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JPS6367141B2 - - Google Patents
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JPS6367141B2 - - Google Patents

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Publication number
JPS6367141B2
JPS6367141B2 JP56063995A JP6399581A JPS6367141B2 JP S6367141 B2 JPS6367141 B2 JP S6367141B2 JP 56063995 A JP56063995 A JP 56063995A JP 6399581 A JP6399581 A JP 6399581A JP S6367141 B2 JPS6367141 B2 JP S6367141B2
Authority
JP
Japan
Prior art keywords
speed
pole
permanent magnet
circuit
voltage
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
Application number
JP56063995A
Other languages
Japanese (ja)
Other versions
JPS57179665A (en
Inventor
Takashi Myazawa
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.)
Daiichi Components Ltd
Original Assignee
Shinano Electric Co Ltd
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 Shinano Electric Co Ltd filed Critical Shinano Electric Co Ltd
Priority to JP56063995A priority Critical patent/JPS57179665A/en
Publication of JPS57179665A publication Critical patent/JPS57179665A/en
Publication of JPS6367141B2 publication Critical patent/JPS6367141B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/44Devices characterised by the use of electric or magnetic means for measuring angular speed
    • G01P3/46Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring amplitude of generated current or voltage

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)

Description

【発明の詳細な説明】 本発明は360゜の回転角度において回転速度に比
例した電圧を得ることができる、小形安価な回転
機の速度検出装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a small and inexpensive speed detection device for a rotating machine that can obtain a voltage proportional to the rotation speed at a rotation angle of 360 degrees.

各種機器の回転角度制御に使用される回転機例
えばステツピングモータのように、360゜以下の回
転が行われることが殆どのものにあつては、その
速度の検出は回転角度内において行えば足りるも
のであつて、従来のタコジエネレータのような速
度検出装置、即ち360゜回転における速度の検出を
目的とした大形高価なものを使用する必要は全く
ない。このため従来から上記の要求に合致する速
度検出装置が種々提案されているが、これらは製
造が複雑であつて高価であつたり、速度に比例し
た電圧の取出し角度範囲が狭いなどの性能上の難
点があり、満足できるものではない。
For most rotating machines used to control the rotation angle of various devices, such as stepping motors, which rotate less than 360 degrees, it is sufficient to detect the speed within the rotation angle. There is no need to use a conventional speed detection device such as a tachogenerator, that is, a large and expensive device for the purpose of detecting speed in 360° rotation. For this reason, various speed detection devices that meet the above requirements have been proposed, but these devices are complicated and expensive to manufacture, or have performance problems such as a narrow angle range for taking out voltage proportional to speed. It has its drawbacks and is not satisfactory.

そこで本発明者等は上記のような欠点を解決し
た以下に説明する原理の速度検出装置を提案した
(特願昭56―30524号参照)。この装置は第1図a
に示す平面図のように、要求される速度検出角度
に対応した角度だけ例えばN極に着磁し、残りを
S極に着磁した永久磁石円板aを、第1図b,c
に示す平面図および縦断面図のように1点にトロ
イダル状に巻かれた発電コイルbをもつ固定円板
cに対向して設けて、被速度検出回転機に直結の
回転軸dにより、同軸的に回転するように形成し
たものである。この装置は固定された発電コイル
bに鎖交する磁束の大きさおよび極性が、永久磁
石円板aにおけるN,S極の着磁角度と回転速度
(角速度)に対応して変化し、しかも着磁部の磁
束の強さが一定であることを利用して、発電コイ
ルbから例えば第2図a,bに示すような電圧を
取出し(a図はN極の着磁範囲が180゜,b図は
270゜の場合である。)、第2図a,b中の斜線部分
のようにN極の着磁角度範囲、即ち被速度検出回
転機の回転角度だけ回転速度に比例した電圧を取
出して速度の検出を行うものである。従つてN極
の着磁角度を検出すべき回転角度に応じて調節す
れば、任意所望の回転角度内における速度信号を
取出すことが理論上可能である。しかし実際上発
電コイルbを幅をもたないように巻回することは
不可能であつて、永久磁石円板aのN極とS極か
らの磁束が同時に鎖交するのをまぬがれることが
できない。その結果例えば第2図a′,b′に示す波
形図のように、NからS,SからNへの交換点に
おいて波形がなまるため、電圧が回転速度に比例
する範囲は180゜の場合において150゜、また270゜の
場合において240゜程度であつて、前後15゜程度の
範囲においては速度に比例した電圧を取出すこと
はできず、被速度検出回転機の回転角度の全域に
おいて、速度に比例した電圧を取出すことができ
ない。また原理上S極の着磁をなくすことはでき
ないため、N極の最大着磁角度は360゜以下となら
ざるを得ず実際上330゜前後となる。このため波形
のなまる角度を15゜とした場合、速度に比例した
電圧を取出しうる最大の回転角度は315゜以下とな
り、それ以上のものに対しては検出できないこと
になる。従つてこの装置が従来のものに比べて
360゜以下の広い回転角度範囲に亘つて速度を検出
できることは事実であるがまだ不十分である。
Therefore, the present inventors have proposed a speed detection device based on the principle described below, which solves the above-mentioned drawbacks (see Japanese Patent Application No. 56-30524). This device is shown in Figure 1a.
As shown in the plan view shown in Fig. 1, a permanent magnet disk a is magnetized, for example, to the north pole at an angle corresponding to the required speed detection angle, and the remaining part is magnetized to the south pole.
As shown in the plan view and vertical cross-sectional view shown in Fig. 2, it is installed opposite to a fixed disk c having a generating coil b wound in a toroidal shape at one point, and is coaxially It is designed to rotate. In this device, the magnitude and polarity of the magnetic flux linked to the fixed generator coil b change in accordance with the magnetization angle and rotational speed (angular velocity) of the N and S poles of the permanent magnet disk a. Taking advantage of the fact that the strength of the magnetic flux in the magnetic part is constant, a voltage as shown in Figure 2 a and b is obtained from the generator coil b (Figure a shows the magnetization range of the N pole is 180°, b The diagram is
This is the case at 270°. ), the speed is detected by extracting a voltage proportional to the rotational speed within the magnetization angle range of the N pole, that is, the rotational angle of the speed-detected rotating machine, as shown by the shaded areas in Figure 2 a and b. . Therefore, by adjusting the magnetization angle of the N pole according to the rotation angle to be detected, it is theoretically possible to extract a speed signal within any desired rotation angle. However, in practice, it is impossible to wind the generator coil b so that it has no width, and it is impossible to avoid simultaneous interlinkage of the magnetic fluxes from the N and S poles of the permanent magnet disk a. . As a result, as shown in the waveform diagrams shown in Figure 2 a' and b', the waveform becomes dull at the exchange points from N to S and from S to N, so the range in which the voltage is proportional to the rotational speed is 180°. When the angle is 150°, and when the angle is 270°, it is about 240°, and it is not possible to extract a voltage proportional to the speed in a range of about 15° before and after. It is not possible to extract a voltage proportional to . Furthermore, since it is impossible in principle to eliminate the magnetization of the S pole, the maximum magnetization angle of the N pole must be 360° or less, and in practice it is around 330°. Therefore, if the rounding angle of the waveform is 15 degrees, the maximum rotation angle at which a voltage proportional to speed can be extracted is 315 degrees or less, and anything larger than that cannot be detected. Therefore, this device is more effective than conventional ones.
Although it is true that speed can be detected over a wide rotation angle range of 360° or less, it is still insufficient.

本発明は以上のような速度検出原理を応用し
て、360゜の回転において速度に比例した電圧を取
出しうる小形安価な速度検出装置の実現を図つた
もので、次に図面を用いてその詳細を説明する。
The present invention applies the speed detection principle described above to realize a small and inexpensive speed detection device that can extract a voltage proportional to the speed during 360° rotation. Explain.

第3図a,bは本発明装置の一実施例を示す縦
断面図および回路図、第4図a,bは永久磁石回
転円板の平面図および固定円板の平面図および永
久磁石回転円板の磁極を検出する素子の設置位置
を示す平面図であつて、その特徴とするところは
次の点にある。即ち固定円板に180゜の角度を隔て
て第1、第2の発電コイルを設け、180゜位相の異
なる第1、第2の速度検出電圧が得られるように
形成すると共に、永久磁石回転円板の回転と同期
して上記第1、第2の速度検出電圧から180゜の範
囲に亘つてその回転速度に比例する電圧部分のみ
を選択取得するための制御信号発生回路と、その
選択取得電圧の合成回路を設けて、360゜の回転角
度全域において速度に比例する電圧を取出し得る
ようにした点にある。
FIGS. 3a and 3b are longitudinal cross-sectional views and circuit diagrams showing one embodiment of the device of the present invention, and FIGS. 4a and 4b are plan views of a permanent magnet rotating disk, a plan view of a fixed disk, and a permanent magnet rotating circle. It is a plan view showing the installation position of an element for detecting the magnetic pole of a plate, and its features are as follows. That is, first and second power generation coils are provided on a fixed disk at an angle of 180 degrees, and are formed so as to obtain first and second speed detection voltages with a phase difference of 180 degrees. A control signal generating circuit for selectively acquiring only a voltage portion proportional to the rotational speed over a range of 180 degrees from the first and second speed detection voltages in synchronization with the rotation of the plate, and the selective acquisition voltage thereof. The point is that a composite circuit is provided to extract a voltage proportional to the speed over the entire rotation angle of 360 degrees.

第3図において1は回転軸で、ケースを形成す
る部分2,3に設けた軸受4,5によつて支承さ
れ、その突出端は図示しない被速度検出回転機軸
に連結される。6はドーナツ状の永久磁石回転円
板で、例えば第4図aに示すように270゜の角度範
囲にN極が着磁され、残りの90゜の範囲がS極に
着磁されており、高導磁率材製のヨーク円板7に
より回転軸1に固定される。8はドーナツ状の固
定円板で高導磁率材で作られる。9,10は第1
および第2の発電コイルで、第4図bに示すよう
に固定円板8の180゜の角度を隔てた2点にトロイ
ダル状に巻かれる。そして固定円板8は永久磁石
回転円板6と少ない空隙を隔てて同軸的に対向す
るようにケース部分3上に固定される11,12
(12はかくれて見えない。)は永久磁石回転円板
の磁極を検出する第1、第2磁気感応素子で、例
えばホール素子のような磁気感応素子が用いられ
る。そして第4図aによつて前記したようにN極
の着磁角度が270゜の場合には、第4図bのように
第1発電コイル9の設置点を中心として、これよ
り反時計方向および時計方向のそれぞれ45゜の点
に位置するように、永久磁石回転円板6に近接し
てケース部分3上に固定されるもので、設置角度
はN極の着磁角度をθとしたとき、一般に θ−180゜/2 によつて与えられる。また第3図において13,
14は第1および第2の位相検波回路、15は電
圧選択合成回路で、第1、第2位相検波回路1
3,14には上記磁気感応素子11,12の出力
が加えられ、またその出力はアンドがとられるよ
うに接続される。そしてアンド出力は第1および
第2発電コイル9,10の出力が加えられている
電圧選択合成回路15に加えられる。16は速度
に比例する電圧信号の出力端子である。
In FIG. 3, reference numeral 1 denotes a rotating shaft, which is supported by bearings 4 and 5 provided in parts 2 and 3 forming the case, and its protruding end is connected to a speed-detected rotary machine shaft (not shown). 6 is a donut-shaped permanent magnet rotating disk, for example, as shown in Figure 4a, the north pole is magnetized in an angular range of 270°, and the remaining 90° range is magnetized as a south pole; It is fixed to the rotating shaft 1 by a yoke disk 7 made of a high magnetic permeability material. 8 is a donut-shaped fixed disk made of high magnetic permeability material. 9 and 10 are the first
A second generating coil is wound in a toroidal manner at two points separated by an angle of 180 degrees on the fixed disk 8, as shown in FIG. 4b. The fixed disk 8 is fixed on the case portion 3 so as to coaxially face the permanent magnet rotating disk 6 with a small gap between them 11 and 12.
(12 is hidden and cannot be seen) are first and second magnetically sensitive elements that detect the magnetic poles of the permanent magnet rotating disk, and for example, a magnetically sensitive element such as a Hall element is used. If the magnetization angle of the N pole is 270° as described above with reference to FIG. 4a, then as shown in FIG. It is fixed on the case part 3 in close proximity to the permanent magnet rotating disk 6 so as to be located at a point of 45 degrees clockwise, and the installation angle is when the magnetization angle of the N pole is θ. , generally given by θ−180°/2. Also, in Figure 3, 13,
14 is a first and second phase detection circuit, 15 is a voltage selection and synthesis circuit, and the first and second phase detection circuit 1
The outputs of the magnetically sensitive elements 11 and 12 are added to 3 and 14, and the outputs are connected so as to be ANDed. The AND output is then applied to a voltage selection and synthesis circuit 15 to which the outputs of the first and second generator coils 9 and 10 are added. 16 is an output terminal for a voltage signal proportional to speed.

次にこの装置の動作を第5図に示す波形図を参
照して説明する。永久磁石回転円板6が回転軸1
により第4図a中の矢印Aの方向に回転されたも
のとする。すると第1発電コイル9からは前記し
た原理により、第5図aに示す波形の電圧E1
送出され、また第2発電コイル10からは第5図
bに示すようにE1と180゜位相の異なる出力電圧E2
が送出されて、そのそれぞれは電圧選択合成回路
15に加えられる。一方第1、第2磁気感応素子
11,12は永久磁石回転円板6からの磁束に感
応してN極に着磁された角度範囲即ち270゜の間は
例えば正極性電圧S極の着磁角度範囲である90゜
の間においては負極性電圧に変換して検出する
が、こゝで上記したように第1、第2磁気感応素
子11,12は、第1発電コイル9を中心として
45゜進んだ点と遅れた点に設けられている。従つ
て第5図cに示すように第1磁気感応素子11か
らは、第1発電コイル9の出力電圧E1と同期し
て、これより45゜位相の進んだ電圧E3が得られ、
また第2磁気感応素子12からはE1より45゜遅れ
た第5図dの電圧E4が出力される。そしてこれ
らE3,E4は第1、第2位相検波回路13,14
に加えられて、その出力にE3,E4の正極性のと
き“1”、負極性のとき“0”となる第5図e,
fの位相検波出力E3′,E4′が送出される。そして
これらはアンドをとられて第5図gに示す電圧選
択取得制御信号E5が得られ、これが電圧選択合
成回路15に加えられるが、こゝで電圧E3′は第
1発電コイル9の出力電圧E1に対して45゜進んで
おり、またE4′はE1に対して45゜だけ遅れている。
従つてアンド出力E5は第5図gに示すようにE1
より45゜遅れた点で立上り、225゜の点で立下つて
零となり、再び405゜で立上つて585゜で立下つて零
となる、ハイレベルとローレベル信号とから形成
される角度幅がそれぞれ180゜の選択取得制御信号
となる。このように磁気感応素子11,12と位
相検波回路13,14の出力のアンド回路が選択
取得制御信号発生回路となる。従つて電圧選択合
成回路15において、ハイレベル信号Hが加えら
れたとき第1発電コイル9の出力E1をサンプル
し、またローレベル信号Lが加えられたとき第2
発電コイル10の出力E2をサンプルすれば、第
5図hに示すように第1発電コイル9の出力E1
の45゜から225゜の間の回転速度に正しく比例する
電圧EAが得られ、また第2発電コイル10の出
力E2においては225゜から405゜の間の回転速度に正
しく比例する電圧EBが得られる。そして以下同
じ要領でサンプリング動作が行われ、360゜の間連
続的に回転速度に正しく比例した速度検出電圧信
号E6が得られることになる。
Next, the operation of this device will be explained with reference to the waveform diagram shown in FIG. The permanent magnet rotating disk 6 is the rotating shaft 1
Assume that it is rotated in the direction of arrow A in FIG. 4a. Then, according to the above - described principle, the first generating coil 9 sends out a voltage E 1 with the waveform shown in FIG. Different output voltages of E 2
are sent out, and each of them is applied to the voltage selection and synthesis circuit 15. On the other hand, the first and second magnetically sensitive elements 11 and 12 are magnetized to the north pole in response to the magnetic flux from the permanent magnet rotating disk 6 within an angular range of 270 degrees, for example, with a positive polarity voltage S pole magnetization. In the angular range of 90 degrees, the voltage is converted to negative polarity and detected, but as described above, the first and second magnetically sensitive elements 11 and 12 are centered around the first generating coil 9.
They are set at points that have advanced 45 degrees and points that have delayed 45 degrees. Therefore, as shown in FIG. 5c, a voltage E 3 is obtained from the first magnetic sensing element 11 in synchronization with the output voltage E 1 of the first generating coil 9 and whose phase is 45° ahead of the output voltage E 1 .
Further, the second magnetically sensitive element 12 outputs a voltage E4 shown in FIG. 5d, which is delayed by 45 degrees from E1 . These E 3 and E 4 are the first and second phase detection circuits 13 and 14.
5 e, whose output becomes "1" when E 3 and E 4 have positive polarity, and "0" when they have negative polarity.
Phase detection outputs E 3 ′ and E 4 ′ of f are transmitted. These are ANDed to obtain the voltage selection acquisition control signal E 5 shown in FIG. It leads the output voltage E 1 by 45°, and E 4 ′ lags E 1 by 45°.
Therefore, the AND output E 5 becomes E 1 as shown in Figure 5g.
The angular width formed by the high level and low level signals rises at a point 45 degrees later than that, falls at a point of 225 degrees and becomes zero, rises again at 405 degrees, falls at 585 degrees and becomes zero. are respectively 180° selective acquisition control signals. In this way, the AND circuit of the outputs of the magnetically sensitive elements 11 and 12 and the phase detection circuits 13 and 14 becomes a selection acquisition control signal generation circuit. Therefore, in the voltage selection and synthesis circuit 15, when the high level signal H is applied, the output E1 of the first generating coil 9 is sampled, and when the low level signal L is applied, the output E1 of the first generating coil 9 is sampled.
If the output E 2 of the generator coil 10 is sampled, the output E 1 of the first generator coil 9 will be obtained as shown in FIG. 5h.
A voltage E A is obtained which is correctly proportional to the rotational speed between 45° and 225°, and a voltage E A which is correctly proportional to the rotational speed between 225° and 405° is obtained at the output E 2 of the second generating coil 10. B is obtained. Thereafter, sampling operations are performed in the same manner, and a speed detection voltage signal E6 that is correctly proportional to the rotational speed is obtained continuously over 360 degrees.

従つて本発明によれば第2の発電コイルの付加
と、現在の技術によれば十分小型に形成しうる電
子処理回路の付加による簡単な構造により、第1
図に示した本発明者等によつて提案されたものの
ように速度、検出に当つて不感帯を生ずることな
く、しかも従来のタコゼエネレータと同様に360゜
の回転角度における速度を検出できる小形安価な
速度検出装置を提供できる。また永久磁石回転円
板6は軽量に作ることができるので、従来のタコ
ゼエネレータに比べて慣性を少なくでき、被速度
検出回転機の慣性が大きくて制御の行過ぎを生ず
るようなおそれも少ない。
Therefore, according to the present invention, the first generator coil can be replaced with a simple structure by adding a second generator coil and an electronic processing circuit that can be formed sufficiently small according to current technology.
Like the one proposed by the present inventors shown in the figure, it is a small and inexpensive device that does not create a dead zone when detecting speed, and can also detect speed at a rotation angle of 360° in the same way as a conventional tachoze generator. A detection device can be provided. Furthermore, since the permanent magnet rotating disk 6 can be made lightweight, its inertia can be reduced compared to a conventional tachometer generator, and there is less risk of excessive control due to the large inertia of the speed-detected rotary machine.

以上本発明を永久磁石回転円板6のN極の着磁
角度を270゜、残りをS極に着磁した例について説
明したが、理論上N極の着磁角度が180゜以上であ
れば、何度であつても360゜の間速度に比例した電
圧信号を得ることができるが(180゜に近い方が大
きな出力が得られる)、製作上の精度や後記する
被速度検出回転機の振動による悪影響を除くよう
に考慮した場合などにおいては、N極の着磁角度
は270゜前後がよい。また以上ではN極の着磁角度
を180゜以上としたが、N,Sの角度幅を逆にして
もよい。
The present invention has been described above with reference to an example in which the N pole of the permanent magnet rotating disk 6 is magnetized at an angle of 270 degrees and the rest is magnetized at S poles.However, theoretically, if the magnetization angle of the N pole is 180 degrees or more, , it is possible to obtain a voltage signal proportional to the speed over a 360° angle (the closer to 180°, the greater the output), but due to manufacturing accuracy and speed detection rotating machine described later. When consideration is given to eliminating the adverse effects of vibration, the magnetization angle of the N pole is preferably around 270°. Further, in the above description, the magnetization angle of the N pole was set to be 180° or more, but the angular widths of the N and S poles may be reversed.

また本発明の検出装置では被速度検出回転機が
パルスモータのような振動を生じ易いものの場
合、その振動が第5図hの電圧信号EAとEBの切
り替り時に発生したとき、速度検出電圧信号E6
中に雑音電圧を生じさせる。このため例えばE6
を用いてパルスモータの速度を帰還制御しようと
する場合において、制御の行過ぎなどを生じて制
御精度を低下するおそれがある。即ち振動が回転
軸1を通して永久磁石回転円板6に伝達されるた
め、その振動に対応して第1、第2発電コイル
9,10の出力電圧E1,E2、第1、第2位相検
波回路13,14のアンド出力E5(選択取得制御
信号)もその立下り点において振動するため、第
5図h中に点線で示すように雑音電圧ENを生ず
ることになり、上記のような欠点を生ずることに
なる。しかしこれは第1、第2位相検波回路1
3,14のアンド出力に、振動角度幅以上の角度
幅をもつヒステリシス特性、例えば10゜のヒステ
リシス特性をもたせることによつて防ぐことがで
きる。例えば前記した実施例では回転軸1の左右
何れの方向の回転の場合にも、45゜〜225゜までの
間第1発電コイル9の出力電圧E1をサンプルし、
225゜〜405゜の間第2発電コイル10の出力電圧E2
をサンプルするようにした。しかし第5図g中に
示すように10゜のヒステリシスをもたせるように
して、時計方向の回転のとき50゜〜230゜まで第1
発電コイル9の出力電圧E1を、また230゜〜410゜の
間第2発電コイル10の出力電圧E2をサンプル
するようにし、反時計方向の回転のときには40゜
〜220゜の間E1を、220゜〜400゜の間E2をサンプルす
るようにすれば、パルスモータの振動による影響
を除くことができる。
In addition, in the detection device of the present invention, when the speed-detected rotating machine is one that easily generates vibrations such as a pulse motor, when the vibration occurs at the time of switching between the voltage signals E A and E B shown in Fig. 5h, the speed is detected. Voltage signal E 6
generates noise voltage inside. For example E 6
When attempting to perform feedback control of the speed of the pulse motor using the above-mentioned method, there is a risk that the control may be over-controlled and the control accuracy may be reduced. That is, since vibrations are transmitted to the permanent magnet rotating disk 6 through the rotating shaft 1, the output voltages E 1 and E 2 of the first and second generator coils 9 and 10 and the first and second phases are changed in response to the vibrations. Since the AND output E 5 (selection acquisition control signal) of the detection circuits 13 and 14 also oscillates at its falling point, a noise voltage E N is generated as shown by the dotted line in Fig. 5h, and as described above. This will result in significant drawbacks. However, this is because the first and second phase detection circuits 1
This can be prevented by providing the AND outputs of 3 and 14 with a hysteresis characteristic having an angular width greater than the vibration angular width, for example, a hysteresis characteristic of 10 degrees. For example, in the embodiment described above, the output voltage E 1 of the first generator coil 9 is sampled between 45° and 225° when the rotating shaft 1 rotates in either the left or right direction.
The output voltage E 2 of the second generating coil 10 between 225° and 405°
I tried to sample it. However, as shown in Figure 5g, by providing a hysteresis of 10°, the first
The output voltage E 1 of the generator coil 9 is sampled, and the output voltage E 2 of the second generator coil 10 is sampled between 230° and 410°, and during counterclockwise rotation, the output voltage E 1 is sampled between 40° and 220°. By sampling E 2 between 220° and 400°, the influence of pulse motor vibration can be removed.

また以上では選択取得制御信号発生回路素子と
して磁気感応素子を用いた例を示したが、ホトト
ランジスタのような光感応素子を用いても実施で
きる。この方法は例えば第6図a,bに示す要部
側面図および平面図(第3図と同一符号は同等部
分を示す)のように、ヨーク円板7の直径を永久
磁石回転円板6のそれより大として、その周縁の
180゜の範囲に亘つて設けた切欠き17を挾みこむ
ように、光源18と光感応素子19を対向して設
けると同時に(切欠き17を設けることなくこれ
に対応してミラーを設けて、光源からの光をこれ
に反射させて光感応素子に与えるようにしてもよ
い)、その光感応素子の設置位置を磁気感応素子
と同様に、N極の着磁角度を例えば270゜としたと
き、第6図bに示すように第1発電コイル9の設
置点から45゜遅れた点に固定して、磁気感応素子
を用いたと同様な作用を行わせるものである。即
ち永久磁石回転円板6が図示の位置から第6図b
の矢印の方向に回転して、切欠き17により光源
18からの光が光感応素子19に達すると、第5
図a,gに示したと同様に第1発電コイル9の出
力電圧E1に対して45゜遅れた点から180゜間隔で
“1”“0”に変化する光感応素子の出力が選択取
得制御信号E5として得られることなる。そこで
これを第7図に示す回路図のように電圧選択合成
回路15に加えて前記した要領により出力電圧
E1とE2とをサンプルして合成すれば、第5図h
に示したと同様に360゜の回転角度に亘つて速度に
比例した電圧信号E6を得ることができる。従つ
てこの方法によれば光検出素子が1箇ですみ、位
相検波回路も必要としないので、磁気感応素子を
用いる場合に比べて、速度検出装置を更に小形安
価に構成できる。
Moreover, although an example in which a magnetically sensitive element is used as the selective acquisition control signal generating circuit element has been shown above, the present invention can also be implemented using a photosensitive element such as a phototransistor. In this method, for example, the diameter of the yoke disk 7 is set to the diameter of the permanent magnet rotating disk 6, as shown in the side view and plan view of the main parts shown in FIGS. Larger than that, the surrounding area
At the same time, the light source 18 and the photosensitive element 19 are provided facing each other so as to sandwich the notch 17 provided over a range of 180 degrees (without providing the notch 17, a corresponding mirror is provided, and the light source (The light from the magnetic field may be reflected and applied to the photosensitive element), and when the photosensitive element is installed at the same position as the magnetically sensitive element, and the magnetization angle of the N pole is set to, for example, 270 degrees, As shown in FIG. 6b, the coil is fixed at a point delayed by 45 degrees from the installation point of the first generating coil 9, and the same effect as using a magnetic sensing element is produced. That is, the permanent magnet rotating disk 6 is moved from the position shown in FIG. 6b.
When the light from the light source 18 reaches the photosensitive element 19 through the notch 17 by rotating in the direction of the arrow, the fifth
As shown in Figures a and g, the output of the photosensitive element changes from "1" to "0" at 180° intervals from a point delayed by 45° with respect to the output voltage E 1 of the first generating coil 9. The signal E will be obtained as 5 . Therefore, as shown in the circuit diagram shown in FIG. 7, this is added to the voltage selection and synthesis circuit 15, and the output voltage is
If E 1 and E 2 are sampled and synthesized, Figure 5 h
A voltage signal E 6 proportional to the speed can be obtained over a rotation angle of 360° as shown in FIG. Therefore, according to this method, only one photodetection element is required and no phase detection circuit is required, so the speed detection device can be constructed more compactly and inexpensively than when a magnetically sensitive element is used.

以上の説明から明らかなように、本発明によれ
ば360゜回転角度における回転速度を検出できる構
造簡単、小形安価な速度検出装置を提供できるも
ので、実用上の効果は著しい。
As is clear from the above description, according to the present invention, it is possible to provide a speed detection device with a simple structure, small size, and low cost that can detect the rotation speed at a rotation angle of 360 degrees, and the practical effects are remarkable.

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

第1図a,b,cは従来の速度検出装置を示す
永久磁石円板の平面図、固定円板の平面図および
縦断面図、第2図a,b,a′,b′はその動作を説
明するための波形図、第3図a,bは本発明の一
実施例を示す装置の縦断面図および回路図、第4
図a,bは永久磁石固定円板の平面図および固定
円板の平面図、第5図は第3図bの回路図におけ
る各部の波形図、第6図a,bは光感応素子によ
る例を示す本発明装置の要部縦断面図および要部
平面図、第7図は第6図装置の回路図である。 1…回転軸、2,3…ケース部分、4,5…軸
受、6…ドーナツ状永久磁石円板、7…ヨーク円
板、8…ドーナツ状固定円板、9,10…第1、
第2発電コイル、11,12…第1、第2磁極位
置検出素子(磁気感応素子)、13,14…第1、
第2位相検波回路、15…電圧選択合成回路、1
6…出力端子、17…切欠き、18…光源、19
…光感応素子。
Figures 1 a, b, and c are a plan view of a permanent magnet disk, a plan view, and a vertical sectional view of a fixed disk, showing a conventional speed detection device, and Figures 2 a, b, a', and b' are its operation. FIGS. 3a and 3b are a vertical cross-sectional view and a circuit diagram of a device showing an embodiment of the present invention, and FIG. 4 is a waveform diagram for explaining the
Figures a and b are a plan view of the permanent magnet fixed disk and a plan view of the fixed disk, Figure 5 is a waveform diagram of each part in the circuit diagram of Figure 3 b, and Figures 6 a and b are examples using photosensitive elements. FIG. 7 is a circuit diagram of the device shown in FIG. 6. DESCRIPTION OF SYMBOLS 1... Rotating shaft, 2, 3... Case part, 4, 5... Bearing, 6... Donut-shaped permanent magnet disk, 7... Yoke disk, 8... Donut-shaped fixed disk, 9, 10... First,
Second power generation coil, 11, 12...first and second magnetic pole position detection elements (magnetic sensitive elements), 13, 14...first,
Second phase detection circuit, 15... Voltage selection synthesis circuit, 1
6... Output terminal, 17... Notch, 18... Light source, 19
...Photosensitive element.

Claims (1)

【特許請求の範囲】 1 180゜の角度を隔てて第1、第2発電コイルが
トロイダル状に巻かれた高導磁率性の固定円板
と、これと同軸的に対応して被速度検出回転機に
接続される回転軸により回転され、かつ180゜以上
の角度範囲をN極(またはS極)残りの角度範囲
をS極(またはN極)に着磁された永久磁石回転
円板とを設けて、上記永久磁石回転円板の回転に
よる鎖交磁束にもとづき上記第1、第2発電コイ
ルに180゜位相の異なる電圧が誘起されるように形
成すると共に、上記第1、第2発電コイルのそれ
ぞれの出力電圧から180゜の角度範囲に亘つてその
回転速度に比例する電圧部分を選択取得するため
の制御信号発生回路とその制御信号による第1、
第2発電コイル出力からの選択取得電圧を合成す
る回路とを設けて360゜の回転角度において上記回
転軸の回転速度に比例する信号が得られるように
したことを特徴とする回転機の速度検出装置。 2 特許請求の範囲第1項記載の発明において、
その制御信号発生回路が発電コイルの前後におい
て所定の角度で永久磁石回転円板に近接して固定
された第1、第2の磁気感応素子にそれぞれ誘起
される電圧の組合せ回路で構成されたことを特徴
とする回転機の速度検出装置。 3 特許請求の範囲第1項記載の発明において、
その制御信号発生回路が発電コイルから所定角度
だけ遅れた位置に固定され、永久磁石回転円板の
回転に際してその180゜の角度範囲だけ受光するよ
うに装置された光感応素子回路で構成されたこと
を特徴とする回転機の速度検出装置。 4 特許請求の範囲第1項の発明において、その
制御信号発生回路の出力にヒステリシス特性をも
たせ、その出力電圧の切替位置における被速度検
出回転機の振動による雑音混入を避けるようにし
たことを特徴とする回転機の速度検出装置。
[Claims] 1. A high magnetic permeability fixed disk on which first and second generating coils are wound in a toroidal shape at an angle of 180°, and a speed-detected rotating disk coaxially corresponding thereto. A permanent magnet rotating disk is rotated by a rotating shaft connected to the machine and magnetized with an angular range of 180° or more as N pole (or S pole) and the remaining angular range as S pole (or N pole). so that voltages having a phase difference of 180° are induced in the first and second power generation coils based on the interlinkage magnetic flux caused by the rotation of the permanent magnet rotating disk, and the first and second power generation coils A control signal generating circuit for selectively obtaining a voltage portion proportional to the rotation speed over an angular range of 180° from each output voltage of the
Speed detection of a rotating machine, characterized in that a circuit for synthesizing selectively obtained voltages from the output of the second generating coil is provided so that a signal proportional to the rotational speed of the rotating shaft can be obtained at a rotation angle of 360°. Device. 2 In the invention described in claim 1,
The control signal generation circuit is constituted by a combination circuit of voltages respectively induced in first and second magnetically sensitive elements fixed at a predetermined angle in front and behind the generator coil in close proximity to the permanent magnet rotating disk. A rotating machine speed detection device featuring: 3 In the invention described in claim 1,
The control signal generation circuit is fixed at a position delayed by a predetermined angle from the power generation coil, and is composed of a photosensitive element circuit configured to receive light only within that 180° angular range when the permanent magnet rotating disk rotates. A rotating machine speed detection device featuring: 4. The invention set forth in claim 1 is characterized in that the output of the control signal generation circuit has a hysteresis characteristic to avoid noise contamination due to vibration of the speed-detected rotating machine at the output voltage switching position. Speed detection device for rotating machines.
JP56063995A 1981-04-30 1981-04-30 Detecting device for velocity of rotating machine Granted JPS57179665A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56063995A JPS57179665A (en) 1981-04-30 1981-04-30 Detecting device for velocity of rotating machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56063995A JPS57179665A (en) 1981-04-30 1981-04-30 Detecting device for velocity of rotating machine

Publications (2)

Publication Number Publication Date
JPS57179665A JPS57179665A (en) 1982-11-05
JPS6367141B2 true JPS6367141B2 (en) 1988-12-23

Family

ID=13245355

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56063995A Granted JPS57179665A (en) 1981-04-30 1981-04-30 Detecting device for velocity of rotating machine

Country Status (1)

Country Link
JP (1) JPS57179665A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3921476A1 (en) * 1989-06-30 1991-01-10 Draegerwerk Ag PRESSURE REDUCER WITH CONTROLLED SHUT-OFF DEVICE
CN111366209B (en) * 2020-02-20 2021-09-07 珠海鼎通科技有限公司 Device and method for detecting number of rotations, storage medium and water meter

Also Published As

Publication number Publication date
JPS57179665A (en) 1982-11-05

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