JPH0145263Y2 - - Google Patents
Info
- Publication number
- JPH0145263Y2 JPH0145263Y2 JP12471881U JP12471881U JPH0145263Y2 JP H0145263 Y2 JPH0145263 Y2 JP H0145263Y2 JP 12471881 U JP12471881 U JP 12471881U JP 12471881 U JP12471881 U JP 12471881U JP H0145263 Y2 JPH0145263 Y2 JP H0145263Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic pole
- magnet
- pole tooth
- iron piece
- 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
Links
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 claims description 49
- 229910052742 iron Inorganic materials 0.000 claims description 24
- 230000005284 excitation Effects 0.000 claims description 16
- 230000004907 flux Effects 0.000 claims description 7
- 230000002093 peripheral effect Effects 0.000 claims description 4
- 239000011295 pitch Substances 0.000 description 7
- 238000010586 diagram Methods 0.000 description 4
- 238000000748 compression moulding Methods 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000005281 excited state Effects 0.000 description 1
- 230000001105 regulatory effect Effects 0.000 description 1
- 239000007787 solid Substances 0.000 description 1
Landscapes
- Permanent Magnet Type Synchronous Machine (AREA)
Description
【考案の詳細な説明】
本考案は鉄片回転型の単相ステツプモータに関
する。[Detailed Description of the Invention] The present invention relates to a single-phase step motor of rotating iron piece type.
鉄片回転型の単相ステツプモータは、始動時に
鉄片回転子に生じる磁極がN極となるかS極とな
るかによつて、例えば前者の場合に正回転するの
であれば、後者の場合には1パルス分逆回転した
後に正回転するという欠点があつた。また回転子
の回転トルクは回転子とマグネツトとの間で生じ
る磁束のやりとりで決定されるだけであるから、
起動時におけるトルクは小さく、起動特性が良く
ない等の欠点があつた。 A single-phase step motor of the iron piece rotating type depends on whether the magnetic pole generated in the iron piece rotor at the time of starting is the N pole or the S pole.For example, if the former rotates in the forward direction, the latter rotates normally. It had a drawback that it rotated in the forward direction after rotating backwards for one pulse. Furthermore, since the rotational torque of the rotor is determined only by the exchange of magnetic flux generated between the rotor and the magnets,
The drawbacks were that the torque at startup was small and the startup characteristics were poor.
本考案は叙上の欠点を是正せんとするもので、
新たな磁極歯を設けることにより回転方向を規制
できると共に起動トルクの向上を図ることができ
る単相ステツプモータを提供することを目的とす
る。 This invention aims to rectify the shortcomings mentioned above.
It is an object of the present invention to provide a single-phase step motor in which the direction of rotation can be regulated and the starting torque can be improved by providing new magnetic pole teeth.
以下に、本考案を実施例によつて説明する。第
1図において、1は回転子軸であり、その軸1は
軸受2を介して軟磁性の第1ボス3に対して回転
自在となつており、また第2ボス4を介して鉄片
回転子5が一体化されている。そして、第1ボス
3には円環状の励磁コイル6が固着されると共
に、その励磁コイル6の上辺を覆うように軟磁性
のヨーク7が固着されると共にその内周に8個の
外側磁極歯8が一体に形成されている。9は上面
が上記鉄片回転子5に若干の間隙を介して対面す
るように位置する円環状のマグネツトであり、非
磁性の取付部材10によつて固定されている。 The present invention will be explained below with reference to examples. In FIG. 1, 1 is a rotor shaft, and the shaft 1 is rotatable through a bearing 2 with respect to a first soft magnetic boss 3, and is connected to an iron piece rotor through a second boss 4. 5 are integrated. An annular excitation coil 6 is fixed to the first boss 3, a soft magnetic yoke 7 is fixed to cover the upper side of the excitation coil 6, and eight outer magnetic pole teeth are attached to the inner circumference of the yoke 7. 8 are integrally formed. Reference numeral 9 denotes an annular magnet whose upper surface faces the iron piece rotor 5 with a slight gap therebetween, and is fixed by a non-magnetic mounting member 10.
上記したマグネツト9は、第2図に示すように
放射状となるように周方向にN極とS極が等ピツ
チで交互に8極着磁され、その着磁面が鉄片回転
子5に対面するよう固定配置される。 As shown in FIG. 2, the above-mentioned magnet 9 is magnetized with 8 N poles and S poles alternately arranged at equal pitches in the circumferential direction so as to form a radial pattern, and the magnetized surface faces the iron piece rotor 5. so that it is fixedly placed.
また、鉄片回転子5は、第3図に示すように、
第2ボス4に対する固着部としての内周鍔53が
形成されると共に第1磁極歯51と第2磁極歯52
とが、上記内周鍔53より交互に延長されている。
そして第1磁極歯51は内周鍔52より微少断面積
部54を介して連接されると共に円周方向長さは
第2磁極歯52より長く形成されている。一方第
2磁極歯52は内周鍔53より、該磁極歯52の幅
のまま延長されている。さらに各磁極歯51,52
は未広がりの形状となつていて、夫々が4枚づつ
形成され、かつこの第1磁極歯51と第2磁極歯
52は、前記マグネツト9のN極、S極のピツチ
と同一ピツチで形成されている。 Moreover, the iron piece rotor 5 is, as shown in FIG.
An inner circumferential flange 5 3 is formed as a fixing portion to the second boss 4, and the first magnetic pole tooth 5 1 and the second magnetic pole tooth 5 2 are formed.
and are alternately extended from the inner peripheral collar 53 .
The first magnetic pole tooth 5 1 is connected to the inner peripheral flange 5 2 via a small cross-sectional area portion 5 4 and has a longer circumferential length than the second magnetic pole tooth 5 2 . On the other hand, the second magnetic pole tooth 5 2 extends from the inner peripheral flange 5 3 with the same width as the magnetic pole tooth 5 2 . Furthermore, each magnetic pole tooth 5 1 , 5 2
have an unexpanded shape, and are formed of four pieces each, and the first magnetic pole teeth 51 and the second magnetic pole teeth 52 have the same pitch as the N and S poles of the magnet 9. It is formed.
また、前記外側磁極歯8は、第4図に示すよう
にマグネツト9の磁極ピツチと同一ピツチにて8
個形成されているが、第5図に示すようにそのマ
グネツト9の極中心から若干の角度αだけ反時計
廻り方向にずれるように位相差をもたせた配置と
なつている。 Further, the outer magnetic pole teeth 8 are arranged at the same pitch as the magnetic pole pitch of the magnet 9, as shown in FIG.
As shown in FIG. 5, the magnets 9 are arranged so as to have a phase difference such that they are offset by a slight angle α counterclockwise from the polar center of the magnet 9.
更に、前記励磁コイル6は、第6図に示すよう
に、中間タツプ6aに直流電圧+Bが印加される
形式のもので成り、第1制御端子11に正パルス
が加わることにより第1トランジスタ12が導通
して、その励磁コイル6に実線の矢印方向に電流
が流れ、一方第2制御端子13に正パルスが加わ
ることにより、第2トランジスタ14が導通し
て、その励磁コイル6に破線の矢印方向に電流が
流れるようになつている。そして、これによつて
励磁コイル6に磁束が生じると、その磁束は第1
図の破線で示すループ15、つまり第1ボス3←→
ヨーク7←→外側磁極歯8←→ギヤツプg←→鉄片回転
子5←→第2ボス4←→第1ボス3を流れる。これに
より、鉄片回転子5の第1磁極歯51と第2磁極
歯52に相逆の磁極が誘導され、また長い方の第
1磁極歯51が外側磁極歯8に対して吸引力を受
けるようになる。 Furthermore, as shown in FIG. 6, the excitation coil 6 is of a type in which a DC voltage +B is applied to the intermediate tap 6a, and when a positive pulse is applied to the first control terminal 11, the first transistor 12 is activated. When conductive, a current flows through the excitation coil 6 in the direction of the arrow shown by the solid line.On the other hand, when a positive pulse is applied to the second control terminal 13, the second transistor 14 becomes conductive, and the current flows through the excitation coil 6 in the direction indicated by the dashed arrow. Current is now flowing through. When a magnetic flux is generated in the excitation coil 6 due to this, the magnetic flux is
Loop 15 indicated by the broken line in the figure, that is, the first boss 3←→
It flows through the yoke 7←→outer magnetic pole tooth 8←→gap g←→iron piece rotor 5←→second boss 4←→first boss 3. As a result, opposite magnetic poles are induced in the first magnetic pole tooth 5 1 and the second magnetic pole tooth 5 2 of the iron piece rotor 5, and the longer first magnetic pole tooth 5 1 exerts an attractive force on the outer magnetic pole tooth 8. will begin to receive
次に動作を説明する。上記第1制御端子11に
は第7図Aに示すパルス信号が、また第2制御端
子13には第7図Bに示すパルス信号が各々加え
られるが、両パルス信号A,Bはデユーテイサイ
クルが50%未満で、かつ位相差が180度となつて
いる。したがつて励磁コイル6は電流が流れない
休止時間t0が生じる。 Next, the operation will be explained. A pulse signal shown in FIG. 7A is applied to the first control terminal 11, and a pulse signal shown in FIG. 7B is applied to the second control terminal 13, but both pulse signals A and B are on duty. The cycle is less than 50% and the phase difference is 180 degrees. Therefore, a rest time t 0 occurs in which no current flows through the exciting coil 6.
第8図は鉄片回転子5の第1磁極歯51と第2
磁極歯52、外側磁極歯8、およびマグネツト9
の相互の関係を示す説明用の図である。 FIG. 8 shows the first magnetic pole tooth 51 and the second magnetic pole tooth of the iron piece rotor 5.
magnetic pole tooth 5 2 , outer magnetic pole tooth 8 , and magnet 9
FIG.
第7図における時間の時、この時は無励磁状
態であり、第1磁極歯51と第2磁極歯52はマグ
ネツト9のN極から出てS極に至る磁束通路の磁
気抵抗が最少となる位置、つまりN極とS極をま
たぐ中間位置にて静止している。この時第8図a
に示すように、反時計廻り方向のN極からS極に
向う極間に第1磁極歯51が静止し、同反時計廻
り方向のS極からN極に向う極間に第2磁極歯5
2が静止しているとする。 At the time shown in FIG. 7, the magnet is in a non-excited state, and the first magnetic pole tooth 5 1 and the second magnetic pole tooth 5 2 have the lowest magnetic resistance in the magnetic flux path from the N pole of the magnet 9 to the S pole. It is stationary at a position where it is, that is, an intermediate position straddling the north and south poles. At this time, Figure 8a
As shown in , the first magnetic pole tooth 51 stands still between the poles running from the north pole toward the south pole in the counterclockwise direction, and the second magnetic pole tooth 51 stands between the poles running from the south pole toward the north pole in the counterclockwise direction. 5
Suppose that 2 is at rest.
次に第7図の時間に至り、励磁コイル6が一
方向に励磁されて、第1磁極歯51がN極、第2
磁極歯52がS極になると、第8図bに示すよう
に吸引反発の磁気作用により、N極となつた第1
磁極歯51がマグネツト9のS極上に、またS極
となつた第2磁極歯52がマグネツト9のN極上
に吸引されて反時計廻り方向にマグネツト9の1/
2磁極ピツチ角度だけ回転し、この状態は第1制
御端子11に加わるパルス信号が零になるまで続
く。なお、この時外側磁極歯8は磁束の受渡しに
より第1磁極歯51を吸引する。このため、第1
磁極歯51はマグネツト9のS極の頂上ではなく、
その外側磁極歯8の側(反時計廻り方向)に若干
の角度β(<α)だけ偏つた位置となり、起動ト
ルクは大きなものとなる。 Next, at the time shown in FIG. 7, the exciting coil 6 is excited in one direction, and the first magnetic pole tooth 51 is the N pole, and the second magnetic pole tooth 51 is the N pole.
When the magnetic pole tooth 52 becomes the S pole, the first tooth becomes the N pole due to the magnetic action of attraction and repulsion, as shown in Figure 8b.
The magnetic pole tooth 51 is attracted onto the south pole of the magnet 9, and the second magnetic pole tooth 52 , which has become the south pole, is attracted onto the north pole of the magnet 9, and the magnetic pole tooth 51 is attracted to the north pole of the magnet 9 in the counterclockwise direction.
It rotates by two magnetic pole pitch angles, and this state continues until the pulse signal applied to the first control terminal 11 becomes zero. Note that at this time, the outer magnetic pole tooth 8 attracts the first magnetic pole tooth 5 1 by transferring magnetic flux. For this reason, the first
The magnetic pole tooth 51 is not the top of the S pole of the magnet 9,
The position is shifted by a slight angle β (<α) toward the outer magnetic pole tooth 8 (counterclockwise direction), and the starting torque becomes large.
次に第7図の時間に至ると、励磁コイル6は
無励磁となり、第1磁極歯51と第2磁極歯52の
磁極は消える。この直前上記したような両磁極5
1と52はマグネツト9の極の頂上からβだけ反時
計廻り方向にずれているので、無励磁になること
により、マグネツト9のN極とS極の作用によつ
てその方向にマグネツト9の1/2磁極ピツチ角度
だけ回転し、そのN極とS極をまたぐ極中間で静
止する(第8図c)。 Next, at the time shown in FIG. 7, the excitation coil 6 becomes non-excited, and the magnetic poles of the first magnetic pole tooth 5 1 and the second magnetic pole tooth 5 2 disappear. Just before this, both magnetic poles 5 as mentioned above
1 and 52 are offset counterclockwise by β from the top of the pole of magnet 9, so when the magnet 9 is de-energized, the action of the north and south poles of magnet 9 causes the magnet 9 to move in that direction. It rotates by 1/2 the magnetic pole pitch angle and comes to rest in the middle between the north and south poles (Figure 8c).
次に第7図の時間に至ると、励磁コイル6が
時間の場合と逆方向に励磁され、第1磁極歯5
1がS極、第2磁極歯52がN極になり、マグネツ
ト9の磁極との吸引反発作用により、第8図dに
示すように更に反時計方向に回転して、第8図b
で示したと同じ状態となる。 Next, when the time shown in FIG. 7 is reached, the exciting coil 6 is excited in the opposite direction to the time, and the first magnetic pole tooth 5
1 becomes the S pole, and the second magnetic pole tooth 5 2 becomes the N pole, and due to the attraction and repulsion with the magnetic pole of the magnet 9, it further rotates counterclockwise as shown in FIG. 8 d, and as shown in FIG.
The situation is the same as shown in .
以下時間の経過と共に以上の動作が繰返され
て、鉄片回転子5は第1制御端子11と第2制御
端子13に加わるパルス信号の1周期毎に、マグ
ネツト9の1磁極ピツチのステツプで反時計廻り
方向に回転する。 Thereafter, the above operation is repeated as time passes, and the iron piece rotor 5 rotates counterclockwise in steps of one magnetic pole pitch of the magnet 9 for each period of the pulse signal applied to the first control terminal 11 and the second control terminal 13. Rotate in the circumferential direction.
ところで、以上は第8図aに示す位置で鉄片回
転子5が静止していた状態で第7図の時間に至
つた場合であるが、第8図a′に示すように、マグ
ネツト9の反時計廻り方向のS極からN極に向う
極間に第1磁極歯51が静止し、同反時計廻り方
向のN極からS極に向う極間に第2磁極歯52が
静止している場合には、次に第7図の時間に至
ることにより回転規制が行なわれる。 By the way, the above is a case where the iron piece rotor 5 is stationary at the position shown in FIG. 8a and the time shown in FIG. 7 is reached, but as shown in FIG. The first magnetic pole tooth 5 1 is stationary between the poles going from the S pole to the N pole in the clockwise direction, and the second magnetic pole tooth 5 2 is stationary between the poles going from the N pole to the S pole in the counterclockwise direction. If so, the rotation is restricted at the next time shown in FIG.
すなわち、第1制御端子11に正パルスが生じ
て励磁コイル6が一方向に励磁され、前記の場合
と同様に第1磁極歯51がN極に、第2磁極歯52
がマグネツト9の磁極との吸引反発作用によつて
反時計廻り方向に回転して、第8図b′の位置にく
る。この状態は第8図bと同じであり、以後の無
励磁により第8図cに移行して、その後は前記の
場合と同様に反時計廻り方向にステツプ回転を続
ける。 That is, a positive pulse is generated at the first control terminal 11 and the excitation coil 6 is excited in one direction, so that the first magnetic pole tooth 5 1 becomes the N pole and the second magnetic pole tooth 5 2 becomes the N pole, as in the previous case.
is rotated counterclockwise by attraction and repulsion with the magnetic poles of the magnet 9, and comes to the position shown in FIG. 8b'. This state is the same as that shown in FIG. 8b, and the state shifts to FIG. 8c due to subsequent de-energization, after which step rotation continues in the counterclockwise direction as in the previous case.
以上のように、励磁時に第1磁極歯51が、通
常ならばマグネツト9の磁極の頂上に吸引される
のであるが、本実施例においては第1磁極歯51
が外側磁極歯8にも吸引されるので、その第1磁
極歯51がその外側磁極歯8の側に角度βだけ偏
した位置にて吸引状態が続けられる。したがつて
無励磁になることにより、その外側磁極歯8の側
に回転する。すなわち、鉄片回転子5は、マグネ
ツト9の極上から偏した外側磁極歯8の方向に回
転する。上記の実施例では反時計廻り方向に偏し
ていたので反時計廻り方向に回転することは前述
のとおりであるが、時計廻り方向に偏させればそ
の時計廻り方向に回転する。つまり、外側磁極歯
8の偏する方向によつて鉄片回転子の回転方向が
定まる。 As described above, the first magnetic pole tooth 5 1 is normally attracted to the top of the magnetic pole of the magnet 9 during excitation, but in this embodiment, the first magnetic pole tooth 5 1 is attracted to the top of the magnetic pole of the magnet 9.
Since the first magnetic pole tooth 51 is also attracted to the outer magnetic pole tooth 8, the attracted state continues at a position where the first magnetic pole tooth 51 is deviated by an angle β toward the outer magnetic pole tooth 8. Therefore, by becoming non-energized, it rotates toward the outer magnetic pole tooth 8 side. That is, the iron piece rotor 5 rotates in the direction of the outer magnetic pole teeth 8 which are offset from the top of the magnet 9. In the above embodiment, the rotation is counterclockwise since it is biased in the counterclockwise direction, and as described above, it rotates in the counterclockwise direction, but if it is biased in the clockwise direction, it rotates in the clockwise direction. In other words, the direction of rotation of the iron piece rotor is determined by the direction in which the outer magnetic pole teeth 8 are biased.
なお、以上の実施例において、励磁コイル6が
中間タツプ無しの場合には、第9図に示すよう
に、トランジスタ15〜18によつてブリツジ接続
して、第1制御端子11に加わる正パルス信号に
よつてトランジスタ15と16が導通して励磁コ
イル6に実線の矢印方向の電流が流れ、また第2
制御端子13に加わるパルス信号によつてトラン
ジスタ17と18が導通して励磁コイル6に破線
の矢印方向の電流が流れるようすることもでき
る。 In the above embodiment, if the excitation coil 6 does not have an intermediate tap, as shown in FIG. As a result, transistors 15 and 16 become conductive, and a current flows in the direction of the solid arrow in the exciting coil 6.
It is also possible to make the transistors 17 and 18 conductive by a pulse signal applied to the control terminal 13 so that a current flows through the exciting coil 6 in the direction of the dashed arrow.
また、外側磁極歯8は磁性鉄板プレス加工し
て、ヨーク7から個別的に伸びる形状にするもの
も考えられるが、この場合は第1図に示すギヤツ
プgが大きくなつてトルクの低下を招くので、第
4図に示すように純鉄粉を圧縮成形することによ
り、カツプ状の磁性体7の内周に凸状の外側磁極
歯8を形成した方が良い。 It is also conceivable that the outer magnetic pole teeth 8 are formed by pressing a magnetic iron plate into a shape that extends individually from the yoke 7, but in this case, the gap g shown in Fig. 1 becomes large and the torque decreases. As shown in FIG. 4, it is preferable to form convex outer magnetic pole teeth 8 on the inner periphery of the cup-shaped magnetic body 7 by compression molding pure iron powder.
また、この外側磁極歯8は以上の実施例では第
1磁極歯51の数と同じにしたが、1/2,1/4で構
成することもできる。 Further, in the above embodiment, the number of outer magnetic pole teeth 8 is the same as that of the first magnetic pole teeth 51 , but the number may be 1/2 or 1/4.
また、以上の実施例において、第2磁極歯52
は必ずしも必要ない。 Moreover, in the above embodiment, the second magnetic pole tooth 5 2
is not necessarily necessary.
さらに鉄片回転子5の形状は上記した実施例の
ものに限定されるものではなく、上記と同様な動
作を行える形状のもの全てを含むことは勿論であ
る。 Furthermore, the shape of the iron piece rotor 5 is not limited to that of the above-described embodiment, and of course includes all shapes that can perform the same operation as described above.
以上から本考案によれば、鉄片回転子の磁極歯
が外側磁極歯によつて、励磁時にマグネツトの極
の頂上から外側磁極歯の側に偏して静止するの
で、その外側磁極歯によつて鉄片回転子の回転方
向が一方向に規制されるようになる。 From the above, according to the present invention, the magnetic pole teeth of the iron piece rotor stand still biased from the top of the magnet pole toward the outer magnetic pole teeth during excitation due to the outer magnetic pole teeth. The rotation direction of the iron piece rotor is now restricted to one direction.
また、外側磁極歯と鉄片回転子の第1磁極歯と
の間で発生する吸引力が回転力に加算される方向
に働くため、大きな起動トルクが得られ、従つて
同一トルクの単相ステツプモータであれば、極め
て小型化が図れる等の効果を有するものである。 In addition, since the attractive force generated between the outer magnetic pole teeth and the first magnetic pole tooth of the iron piece rotor acts in the direction of adding to the rotational force, a large starting torque is obtained, and therefore a single-phase step motor with the same torque If so, it has the advantage of being extremely compact.
第1図は本考案の単相ステツプモータの一実施
例の断面図、第2図はマグネツトの平面図、第3
図は鉄片回転子の裏面斜視図、第4図は外側磁極
歯付近の裏面斜視図、第5図は外側磁極歯のマグ
ネツトに対する位置関係の説明図、第6図は励磁
コイルの結線図、第7図は励磁コイルに加えるべ
きパルス信号のタイミングチヤート、第8図は動
作説明図、第9図は励磁コイルの別の例の結線図
である。
1……回転子軸、2……軸受、3……第1ボ
ス、4……第2ボス、5……鉄片回転子、51…
…第1磁極歯、52……第2磁極歯、6……励磁
コイル、7……ヨーク、8……外側磁極歯、9…
…マグネツト、10……取付部材。
Fig. 1 is a sectional view of an embodiment of the single-phase step motor of the present invention, Fig. 2 is a plan view of the magnet, and Fig. 3 is a sectional view of an embodiment of the single-phase step motor of the present invention.
The figure is a rear perspective view of the iron piece rotor, Figure 4 is a rear perspective view of the vicinity of the outer magnetic pole teeth, Figure 5 is an explanatory diagram of the positional relationship of the outer magnetic pole teeth with respect to the magnet, Figure 6 is a wiring diagram of the excitation coil, FIG. 7 is a timing chart of a pulse signal to be applied to the excitation coil, FIG. 8 is an operation explanatory diagram, and FIG. 9 is a wiring diagram of another example of the excitation coil. 1... Rotor shaft, 2... Bearing, 3... First boss, 4... Second boss, 5... Iron piece rotor, 5 1 ...
...First magnetic pole tooth, 5 2 ... Second magnetic pole tooth, 6 ... Exciting coil, 7 ... Yoke, 8 ... Outer magnetic pole tooth, 9 ...
...Magnet, 10...Mounting member.
Claims (1)
磁極歯が形成された鉄片回転子と、周方向に複数
のN・Sの磁極が着磁され、その着磁面が上記磁
極歯に間〓を介して対面するように固定配置され
た環状のマグネツトと、上記鉄片回転子の中心か
ら外方に又は外方から中心に向けて磁束を流すた
めの励磁コイルとで成る単相ステツプモータにお
いて、 上記鉄片回転子の上記磁極歯の外周端近くで且
つ上記マグネツトの極の頂上から若干の角度だけ
偏した角度位置に、上記励磁コイルにより生ずる
上記磁束により磁気誘導されて上記磁極歯を吸引
する別の磁極歯を固定配置したことを特徴とする
単相ステツプモータ。[Claims for Utility Model Registration] An iron piece rotor whose center is fixed to the rotor shaft and a plurality of magnetic pole teeth are formed in the circumferential direction, and a plurality of N and S magnetic poles are magnetized in the circumferential direction. An annular magnet fixedly arranged so that its magnetized surface faces the magnetic pole teeth with a gap in between, and an excitation device for causing magnetic flux to flow outward from the center of the iron piece rotor or from the outside toward the center. In a single-phase step motor consisting of a coil, a magnet is generated near the outer peripheral end of the magnetic pole teeth of the iron piece rotor and at an angular position offset by a slight angle from the top of the pole of the magnet, due to the magnetic flux generated by the excitation coil. A single-phase step motor characterized in that another magnetic pole tooth is fixedly arranged to attract the magnetic pole tooth by being guided.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12471881U JPS5831780U (en) | 1981-08-25 | 1981-08-25 | single phase step motor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP12471881U JPS5831780U (en) | 1981-08-25 | 1981-08-25 | single phase step motor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5831780U JPS5831780U (en) | 1983-03-02 |
| JPH0145263Y2 true JPH0145263Y2 (en) | 1989-12-27 |
Family
ID=29918578
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP12471881U Granted JPS5831780U (en) | 1981-08-25 | 1981-08-25 | single phase step motor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5831780U (en) |
-
1981
- 1981-08-25 JP JP12471881U patent/JPS5831780U/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5831780U (en) | 1983-03-02 |
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