JPS6325903Y2 - - Google Patents
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- Publication number
- JPS6325903Y2 JPS6325903Y2 JP1981194083U JP19408381U JPS6325903Y2 JP S6325903 Y2 JPS6325903 Y2 JP S6325903Y2 JP 1981194083 U JP1981194083 U JP 1981194083U JP 19408381 U JP19408381 U JP 19408381U JP S6325903 Y2 JPS6325903 Y2 JP S6325903Y2
- Authority
- JP
- Japan
- Prior art keywords
- plate
- speed detection
- magnetic flux
- bearing support
- magnetic
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
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- Brushless Motors (AREA)
- Permanent Magnet Type Synchronous Machine (AREA)
Description
【考案の詳細な説明】
この考案は、例えば回転界磁型の無整流子モー
タに付属して、モータの回転数に応じた周波数の
速度信号を発生する無整流子モータに関するもの
である。[Detailed Description of the Invention] This invention relates to a non-commutator motor that is attached to, for example, a rotating field type non-commutator motor and generates a speed signal with a frequency corresponding to the number of rotations of the motor.
従来この種のモータとして第1図に示すものが
あつた。a図は平面図、b図はa図のA−A′線
の断面図である。ただしa図には、モータ軸と軸
受と軸受支持板を省略してある。 A conventional motor of this type is shown in FIG. Figure a is a plan view, and figure b is a sectional view taken along line A-A' in figure a. However, the motor shaft, bearing, and bearing support plate are omitted from FIG.
図において、1は軟磁性材よりなるステータ
板、2は軟磁性材よりなるロータ円板で、外周に
は速度信号を発生させるための凹凸形のギヤが切
られている。3はフライホイール、4,5は軟磁
性材よりなる速度検出板であり、ロータ円板2の
ギヤと同一ピツチの速度信号発生用の凹凸形のギ
ヤがそれぞれロータ円板2のギヤと対向して切ら
れている。6はモータ軸、7,8は速度信号を発
生させるための磁路をつくる励磁用の棒状磁石
(以下FG磁石という。)で、これらはモータ軸か
ら等位置にあり、両FG磁石7,8の起磁力は等
量である。しかし、FG磁石7,8の極性は互い
に逆向きになつており、磁石7はS極が、磁石8
はN極がステータ板1に接するように配置され
る。9,10は磁束変化となつてあらわれる速度
信号を電圧に変換するための速度検出用コイル、
11はステータ板1上に配置されたモータの電機
子コイル、12はこの電機子コイル11に対向す
るロータ界磁磁石であり、複数極に着磁されてい
る。13は軸受、14は軸受支持板、15はスラ
スト軸受である。b図中、一点鎖線は磁路を示
し、矢印は磁束の流れを示す。 In the figure, 1 is a stator plate made of a soft magnetic material, 2 is a rotor disc made of a soft magnetic material, and a concave-convex gear is cut on the outer periphery for generating a speed signal. 3 is a flywheel, 4 and 5 are speed detection plates made of soft magnetic material, and concave and convex gears for generating speed signals having the same pitch as the gears on the rotor disk 2 are opposed to the gears on the rotor disk 2, respectively. It has been cut. Reference numeral 6 indicates a motor shaft, and 7 and 8 indicate excitation bar-shaped magnets (hereinafter referred to as FG magnets) that create a magnetic path for generating a speed signal.These magnets are located at the same position from the motor shaft. The magnetomotive forces of are equal. However, the polarities of FG magnets 7 and 8 are opposite to each other, and magnet 7 has an S pole while magnet 8 has an S pole.
is arranged so that the N pole is in contact with the stator plate 1. 9 and 10 are speed detection coils for converting speed signals appearing as magnetic flux changes into voltage;
11 is an armature coil of the motor disposed on the stator plate 1, and 12 is a rotor field magnet facing the armature coil 11, which is magnetized into a plurality of poles. 13 is a bearing, 14 is a bearing support plate, and 15 is a thrust bearing. In Figure b, the dashed line indicates the magnetic path, and the arrows indicate the flow of magnetic flux.
次に従来の無整流子モータにおける速度検出の
動作を説明する。 Next, the speed detection operation in a conventional commutatorless motor will be explained.
第1図に示すようにロータ円板2には一定のギ
ヤツプを隔てて、2枚の速度検出板4,5が配置
され、またこの2枚の速度検出板4,5とステー
タ板1の間には等量異符号の起磁力を持つFG磁
石7,8がそれぞれ配置されている。モータの回
転速度検出には前記FG磁石7,8を起磁力とし
てステータ板、速度検出板4,5、ロータ円板2
を通る一点鎖線で示す磁路が利用される。 As shown in FIG. 1, two speed detection plates 4 and 5 are arranged on the rotor disk 2 with a certain gap between them, and between these two speed detection plates 4 and 5 and the stator plate 1. FG magnets 7 and 8 having magnetomotive forces of equal magnitude and opposite sign are respectively arranged. To detect the rotational speed of the motor, the FG magnets 7 and 8 are used as magnetomotive force to detect the stator plate, the speed detection plates 4 and 5, and the rotor disc 2.
The magnetic path shown by the dashed line passing through is used.
つまりモータが回転するとロータ円板2と速度
検出板4,5の両方に切られた凹凸形のギヤの歯
型によつて、ロータ円板2と速度検出板4,5の
間の磁気抵抗が周期的に変化し速度検出用コイル
9,10を鎖交する磁束に疎密が生じ、この変化
が速度検出用コイル9,10の出力端子に電圧変
化となつて現われる。この電圧変化分の周波数が
モータの回転速度に比例するため、これを速度信
号とすることができる。 In other words, when the motor rotates, the magnetic resistance between the rotor disk 2 and the speed detection plates 4 and 5 is increased by the uneven gear teeth cut on both the rotor disk 2 and the speed detection plates 4 and 5. The magnetic flux that changes periodically and interlinks the speed detection coils 9 and 10 becomes denser and denser, and this change appears as a voltage change at the output terminals of the speed detection coils 9 and 10. Since the frequency of this voltage change is proportional to the rotational speed of the motor, this can be used as a speed signal.
ところで第1図のような構造は、一般に軸受支
持板14には強度・価格等の面から鉄板などの軟
磁性材が使用されるため、FG磁石7,8を起磁
力とする磁束は前記ロータ円板2を通る磁路の他
に軸受支持板14中の磁路も通る。この時の速度
信号検出用の磁路は第1図b図中の一点鎖線のよ
うな磁路の閉ループを構成しており、この時の磁
路の磁気回路図は第2図のようになる。 By the way, in the structure shown in FIG. 1, since a soft magnetic material such as a steel plate is generally used for the bearing support plate 14 from the viewpoint of strength and cost, the magnetic flux generated by the FG magnets 7 and 8 as magnetomotive force is transferred to the rotor. In addition to the magnetic path passing through the disc 2, a magnetic path also passes through the bearing support plate 14. The magnetic path for speed signal detection at this time constitutes a closed loop of magnetic path as shown by the dashed-dotted line in Figure 1b, and the magnetic circuit diagram of the magnetic path at this time is as shown in Figure 2. .
第2図においてRF1,RF2は速度検出板4,5
とロータ円板2の間のそれぞれの磁気抵抗で、速
度検出板4,5とロータ円板2の両方にそれぞれ
切られたギヤの凹凸により周期的に変化する。と
ころで両方の抵抗値は等量である。そこでRF1=
RF2=RFとおく。R11,R12は速度検出板4,5
と軸受支持板14の間にそれぞれの磁気抵抗で、
2つの抵抗値は等量である。そこでR11=R12=
R1とおく。 In Fig. 2, RF 1 and RF 2 are speed detection plates 4 and 5.
The magnetic resistance between the speed detection plates 4 and 5 and the rotor disk 2 changes periodically due to the unevenness of the gears cut into both the speed detection plates 4 and 5 and the rotor disk 2, respectively. By the way, both resistance values are equal. So RF 1 =
Let RF 2 = RF. R 11 and R 12 are speed detection plates 4 and 5
and the bearing support plate 14 with their respective magnetic resistances,
The two resistance values are equal. So R 11 = R 12 =
Let's set it as R 1 .
Rm1,Rm2はFG磁石7,8のそれぞれの内部
磁気抵抗で、2つの抵抗値は等量である。そこで
Rm1=Rm2=Rmとおく。F11,F12はFG磁石6の
起磁力で、等量である。そこでF11=F12=F1とお
く。9,10は速度検出用のコイルである。 Rm 1 and Rm 2 are the respective internal magnetic resistances of the FG magnets 7 and 8, and the two resistance values are equal. Therefore
Let Rm 1 = Rm 2 = Rm. F 11 and F 12 are magnetomotive forces of the FG magnet 6 and are equal. Therefore, let F 11 = F 12 = F 1 . 9 and 10 are coils for speed detection.
この第2図の磁気回路図の磁束の流れは、図中
の矢印方向である。この磁束の流れからもわかる
ように磁気抵抗R11,R12を通る磁路が、磁気抵
抗RF1,RF2を通る磁路に並列に接続されている
ため、速度検出用コイル9,10と鎖交する磁束
の変化は、磁気抵抗RF1,RF2と磁気抵抗R11,
R12の並列合成抵抗x={(2RFR1)/(RF+
R1)}の変化Δx=2Δ{(RFR1)/(RF+R1)}に
よつて生じることになる。ここで、1つの装置に
おいては磁気抵抗値R1は一定であるのでΔR1=
0である。よつて並列抵抗の変化分はΔx=
{(2R1 2)/(RF+R1)2}ΔRFとなる。従つてモ
ータが薄型化し、速度検出板4,5と軸受支持板
14の間のギヤツプがそれぞれ小さくなつて、磁
気抵抗R11,R12の抵抗値R1が小さくなつた場合
には、上記の並列抵抗の変化分Δxも相乗的に小
さくなるため、速度検出用コイル9,10を鎖交
する磁束の変化も小さくなり、この速度検出用コ
イル9,10より得られる速度信号の出力レベル
が大巾に低下してしまうという欠点があつた。 The flow of magnetic flux in the magnetic circuit diagram of FIG. 2 is in the direction of the arrow in the figure. As can be seen from the flow of magnetic flux, the magnetic path passing through the magnetic resistances R 11 and R 12 is connected in parallel to the magnetic path passing through the magnetic resistances RF 1 and RF 2 . Changes in interlinking magnetic flux are caused by magnetic resistance RF 1 , RF 2 and magnetic resistance R 11 ,
Parallel combined resistance of R 12 x = {(2RFR 1 )/(RF+
R 1 )} is caused by a change Δx=2Δ{(RFR 1 )/(RF+R 1 )}. Here, since the magnetic resistance value R 1 is constant in one device, ΔR 1 =
It is 0. Therefore, the change in parallel resistance is Δx=
{(2R 1 2 )/(RF+R 1 ) 2 }ΔRF. Therefore, when the motor becomes thinner and the gap between the speed detection plates 4 and 5 and the bearing support plate 14 becomes smaller, and the resistance value R 1 of the magnetic resistances R 11 and R 12 becomes smaller, the above-mentioned Since the change in parallel resistance Δx also becomes smaller synergistically, the change in the magnetic flux that interlinks the speed detection coils 9 and 10 also becomes smaller, and the output level of the speed signal obtained from the speed detection coils 9 and 10 increases. The drawback was that the width was significantly reduced.
この考案は上記のような従来のものの欠点を改
善するためになされたもので、速度検出板と軸受
支持板の間に、速度検出板に対してFG磁石と同
極性の起磁力を付与するFG補助磁石を配置する
ことにより、上記並列磁路による悪影響を防止す
るようにした無整流子モータを提供することを目
的としている。 This idea was made in order to improve the drawbacks of the conventional ones as mentioned above, and an FG auxiliary magnet is placed between the speed detection plate and the bearing support plate to give the speed detection plate a magnetomotive force of the same polarity as the FG magnet. It is an object of the present invention to provide a commutatorless motor that prevents the adverse effects of the parallel magnetic path by arranging the parallel magnetic paths.
以下、この考案の無整流子モータを図を用いて
説明する。 Hereinafter, the commutatorless motor of this invention will be explained with reference to the drawings.
第3図において第1図と同一符号は同一または
相当部分を示し、前述したと同様な動作を行う。
16,17はFG補助磁石で、速度検出板4,5
にそれぞれFG磁石7,8の検出板4側の磁極と
同じ極性の極が接するように配置されている。な
お、この2個のFG補助磁石16,17の起電力
は等量である。従つて、本考案の速度発電機内に
は第3図中の一点鎖線の如き磁路の閉ループが形
成され、磁束の流れは図中の矢印の方向となる。
この時の磁路の磁気回路図は第4図のようにな
る。 In FIG. 3, the same reference numerals as in FIG. 1 indicate the same or corresponding parts, and the same operations as those described above are performed.
16 and 17 are FG auxiliary magnets, and speed detection plates 4 and 5
The FG magnets 7 and 8 are arranged so that the poles of the same polarity as the magnetic poles on the detection plate 4 side are in contact with each other. Note that the electromotive forces of these two FG auxiliary magnets 16 and 17 are equal. Therefore, in the speed generator of the present invention, a closed loop of magnetic path as indicated by the dashed line in FIG. 3 is formed, and the magnetic flux flows in the direction of the arrow in the figure.
The magnetic circuit diagram of the magnetic path at this time is as shown in FIG.
図において、RF1,RF2,Rm1,Rm2,F11,
F12,9,10は第2図の同一符号と同一または
相当部分を示す。R21,R22はFG補助磁石16,
17と軸受支持板14の間のそれぞれの磁気抵抗
で、抵抗値は等量である。そこでR21=R22=R2
とおく。Rm′1,Rm′2はFG補助磁石16,17
のそれぞれの内部磁気抵抗で抵抗値は等量であ
る。そこでRm′1=Rm′2=Rm′とおく。F21,F22
はFG補助磁石16,17の起磁力であり、両者
は等量である。そこでF21=F22=F2とおく。第4
図中の矢印は磁束の流れ方向を示している。 In the figure, RF 1 , RF 2 , Rm 1 , Rm 2 , F 11 ,
F 12 , 9, and 10 indicate the same or corresponding parts as the same reference numerals in FIG. R 21 and R 22 are FG auxiliary magnets 16,
17 and the bearing support plate 14, the resistance values are equal. So R 21 = R 22 = R 2
far. Rm′ 1 and Rm′ 2 are FG auxiliary magnets 16 and 17
The resistance value is the same for each internal magnetic resistance. Therefore, let Rm′ 1 = Rm′ 2 = Rm′. F21 , F22
is the magnetomotive force of the FG auxiliary magnets 16 and 17, and both are equal. Therefore, let F 21 = F 22 = F 2 . Fourth
The arrows in the figure indicate the flow direction of magnetic flux.
第3図と第4図の磁束の流れる方向を見るとわ
かるように、FG補助磁石16,17を速度検出
板4,5と軸受支持板14の間にそれぞれ上記の
如き極性で配置したために、本考案の速度発電機
の磁路には、FG磁石7,8の両方を起磁力とす
る速度検出板4からロータ円板2,速度検出板
5,FG磁石8,ステータ板1を通りFG磁石7,
速度検出板4へ向う磁路の閉ループとFG補助
磁石16,17を起磁力とする速度検出板4から
ロータ円板2,速度検出板5,FG補助磁石17,
軸受支持板14を通りFG補助磁石16,速度検
出板4へ向う磁路の閉ループとの2つの閉ルー
プが独立に形成されている。 As can be seen from the direction in which the magnetic flux flows in FIGS. 3 and 4, since the FG auxiliary magnets 16 and 17 are arranged between the speed detection plates 4 and 5 and the bearing support plate 14 with the above polarity, The magnetic path of the speed generator of the present invention includes a speed detection plate 4 which uses both FG magnets 7 and 8 as magnetomotive force, passes through the rotor disk 2, the speed detection plate 5, the FG magnet 8, and the stator plate 1 to the FG magnet. 7,
The closed loop of the magnetic path toward the speed detection plate 4 and the FG auxiliary magnets 16 and 17 serve as magnetomotive force.From the speed detection plate 4, the rotor disk 2, the speed detection plate 5, the FG auxiliary magnet 17,
Two closed loops are formed independently, including a closed loop of a magnetic path passing through the bearing support plate 14 to the FG auxiliary magnet 16 and the speed detection plate 4.
従つて、閉ループのFG磁石7,8を起磁力
として速度検出用コイル9,10と鎖交する磁束
は、軸受支持板14側には回り込まずに速度信号
形成のために切られた速度検出板4,5とロータ
円板2のギヤ間のそれぞれの磁気抵抗RF1,RF2
を通るのみなので、速度検出板4,5と軸受支持
板14の間の磁気抵抗R21,R22の抵抗値R2の大
小にかかわらずに速度検出用コイル9,10から
は、閉ループの速度検出板4,5とロータ円板
2の間の凹凸形に切られたギヤによる磁気抵抗変
化(ΔRF)のみに依存した出力レベルの速度信
号を得ることができる。なお、2個のFG磁石7,
8の起磁力を等量異符号としたことと、また2個
のFG補助磁石16,17の起磁力を等量異符号
にしたことによつて、ステータ板1,ロータ円板
2,軸受支持板14をすべて零磁位に保ち得るた
め、上記FG磁石7,8とFG補助磁石16,17
によつて界磁磁界に磁束むらをつくることはな
い。 Therefore, the magnetic flux linked to the speed detection coils 9, 10 using the closed-loop FG magnets 7, 8 as magnetomotive force does not go around to the bearing support plate 14 side, but instead passes through the speed detection plate which is cut to form a speed signal. 4, 5 and the respective magnetic resistances RF 1 , RF 2 between the gears of the rotor disk 2
Therefore, regardless of the magnitude of the resistance value R 2 of the magnetic resistance R 21 , R 22 between the speed detection plates 4, 5 and the bearing support plate 14, the speed detection coils 9, 10 transmit the closed loop speed. It is possible to obtain a speed signal with an output level that depends only on the change in magnetic resistance (ΔRF) due to the uneven gear between the detection plates 4 and 5 and the rotor disk 2. In addition, two FG magnets 7,
By making the magnetomotive forces of 8 have equal amounts and different signs, and by making the magnetomotive forces of the two FG auxiliary magnets 16 and 17 have equal amounts and different signs, the stator plate 1, rotor disk 2, and bearing support In order to keep all the plates 14 at zero magnetic potential, the FG magnets 7 and 8 and the FG auxiliary magnets 16 and 17
This does not create magnetic flux unevenness in the field magnetic field.
以上のようにこの考案によれば、速度検出板と
軸受支持板の間に速度検出板に対して第1の永久
磁石と同一極性の起磁力を与える第2の永久磁石
を設けたので速度検出用コイルと鎖交する磁束が
軸受支持板を通る磁束によつて悪影響を受けるこ
とがなくなり、薄型化に伴なう速度信号レベルの
低下を防止することができるという効果がある。 As described above, according to this invention, a second permanent magnet is provided between the speed detection plate and the bearing support plate, which gives the speed detection plate a magnetomotive force of the same polarity as the first permanent magnet, so that the speed detection coil The magnetic flux interlinking with the bearing support plate is no longer adversely affected by the magnetic flux passing through the bearing support plate, which has the effect of preventing the speed signal level from decreasing due to thinning.
第1図のa図は従来の速度発電機のモータ軸と
軸受と軸受支持板を取り除いた平面図、第1図の
b図は従来の速度発電機の側断面図、第2図は従
来の速度発電機の磁気回路説明図、第3図は本考
案の速度発電機の側断面図、第4図は本考案の速
度発電機の磁気回路説明図である。
1……ステータ板、2……ロータ円板、3……
ロータフライホイール、4,5……速度検出板、
6……モータ軸、7,8……FG磁石、9,10
……速度検出用コイル、11……電機子コイル、
12……ロータ界磁磁石、13……軸受、14…
…軸受支持板、15……スラスト軸受、16,1
7……FG補助磁石。なお図中、同一符号は同一
または相当部分を示す。
Figure a in Figure 1 is a plan view of a conventional speed generator with the motor shaft, bearing, and bearing support plate removed, Figure b in Figure 1 is a side sectional view of the conventional speed generator, and Figure 2 is a side sectional view of the conventional speed generator. FIG. 3 is a side sectional view of the speed generator of the present invention, and FIG. 4 is an explanatory diagram of the magnetic circuit of the speed generator of the present invention. 1... Stator plate, 2... Rotor disc, 3...
Rotor flywheel, 4, 5...speed detection plate,
6... Motor shaft, 7, 8... FG magnet, 9, 10
... Speed detection coil, 11 ... Armature coil,
12...Rotor field magnet, 13...Bearing, 14...
... Bearing support plate, 15 ... Thrust bearing, 16,1
7...FG auxiliary magnet. In the drawings, the same reference numerals indicate the same or corresponding parts.
Claims (1)
支持された回転軸、ステータ板と軸受支持板の間
で回転軸に取付けられ、外周に凹凸が設けられた
ロータ円板、このロータ円板に取付けられたロー
タ界磁磁石、このロータ界磁磁石に対向して上記
ステータ板上に配置された電機子コイル、上記ス
テータ板と軸受支持板との間でロータ円板の外周
に対向して設けられ、対向面に凹凸が形成された
速度検出板、この速度検出板と上記ステータ板と
の間に配置され、上記ロータ円板と速度検出板と
の間を通流する磁束を発生する第1の永久磁石、
この第1の永久磁石に対向して上記速度検出板と
軸受支持板との間に配置され、ロータ円板と速度
検出板との間を流通する磁束を第1の永久磁石に
よる磁束と同一方向で発生する第2の永久磁石、
及び上記第1永久の磁石により通流する磁束通路
に設けられ、上記磁束の変化に基づいて速度信号
を発生する速度検出用コイルを備えた無整流子モ
ータ。 A rotating shaft supported by a stator plate and a bearing support plate that face each other, a rotor disk that is attached to the rotating shaft between the stator plate and the bearing support plate and has an uneven outer periphery, and a rotor field that is attached to this rotor disk. a magnet, an armature coil disposed on the stator plate facing the rotor field magnet, an armature coil disposed opposite to the outer periphery of the rotor disc between the stator plate and the bearing support plate, and an armature coil disposed on the outer circumference of the rotor disk between the stator plate and the bearing support plate; a speed detection plate having an uneven surface, a first permanent magnet disposed between the speed detection plate and the stator plate, and generating a magnetic flux flowing between the rotor disk and the speed detection plate;
The magnetic flux flowing between the rotor disk and the speed detecting plate is directed in the same direction as the magnetic flux generated by the first permanent magnet. A second permanent magnet generated in
and a non-commutator motor, comprising a speed detection coil that is provided in a magnetic flux path through which the first permanent magnet flows and generates a speed signal based on changes in the magnetic flux.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19408381U JPS58100473U (en) | 1981-12-28 | 1981-12-28 | Commutatorless motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP19408381U JPS58100473U (en) | 1981-12-28 | 1981-12-28 | Commutatorless motor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS58100473U JPS58100473U (en) | 1983-07-08 |
JPS6325903Y2 true JPS6325903Y2 (en) | 1988-07-14 |
Family
ID=30107414
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP19408381U Granted JPS58100473U (en) | 1981-12-28 | 1981-12-28 | Commutatorless motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS58100473U (en) |
Families Citing this family (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2208716B (en) * | 1987-08-12 | 1991-02-27 | Smiths Industries Plc | Speed and torque sensors |
CN109075680B (en) * | 2016-06-24 | 2020-08-14 | 宫林正仁郎 | Rotary generator |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56162955A (en) * | 1980-05-15 | 1981-12-15 | Seiko Instr & Electronics Ltd | Rotor |
-
1981
- 1981-12-28 JP JP19408381U patent/JPS58100473U/en active Granted
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS56162955A (en) * | 1980-05-15 | 1981-12-15 | Seiko Instr & Electronics Ltd | Rotor |
Also Published As
Publication number | Publication date |
---|---|
JPS58100473U (en) | 1983-07-08 |
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