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JPS6048985B2 - polyphase alternating current motor - Google Patents
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JPS6048985B2 - polyphase alternating current motor - Google Patents

polyphase alternating current motor

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Publication number
JPS6048985B2
JPS6048985B2 JP8015777A JP8015777A JPS6048985B2 JP S6048985 B2 JPS6048985 B2 JP S6048985B2 JP 8015777 A JP8015777 A JP 8015777A JP 8015777 A JP8015777 A JP 8015777A JP S6048985 B2 JPS6048985 B2 JP S6048985B2
Authority
JP
Japan
Prior art keywords
circuit
wire
poles
phase
starting
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
JP8015777A
Other languages
Japanese (ja)
Other versions
JPS5415112A (en
Inventor
研三 小倉
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura 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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP8015777A priority Critical patent/JPS6048985B2/en
Publication of JPS5415112A publication Critical patent/JPS5415112A/en
Publication of JPS6048985B2 publication Critical patent/JPS6048985B2/en
Expired legal-status Critical Current

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  • Induction Machinery (AREA)

Description

【発明の詳細な説明】 本発明は分割巻線始動を問題なく行えるよう改良した
電機子巻線を備えた多相交流電動機に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a polyphase alternating current motor with an improved armature winding for problem-free split winding starting.

三相同期電動機などのような多相交流電動機は接続さ
れる電源への影響、駆動する負荷に対する影響、自己の
始動特性などを考慮して種々な始動方法が選定される。
For polyphase AC motors such as three-phase synchronous motors, various starting methods are selected in consideration of the influence on the connected power source, the influence on the driven load, the starting characteristics of the motor itself, etc.

それら始動方法にはリアクトル始動、コンドルフア始動
、始動電動機による始動などがあるが、それらの中に特
殊な装置を必要とせず簡単て始動効率もよい方法として
分割巻線始動かある。分割巻線始動は電機子巻線を数個
の並列回路に分け、始動時には並列回路の一部を使用し
、加速に応じて適宜並列回路を生カルて行く方法てある
。具体的方法については従来多くの方法が知られている
が、その中で比較的極数の多い交流電動機に於て電機子
巻線に二つ以上の並列回路を設け、一つの回路に属する
線輪を幾何学的配置で2群に分け、電機子鉄心上で正反
対の位置に一群づつ配置することにより始動時に磁気的
不平衡を生じさせない方法がある。以下更に具体的な一
例について図面を参照しながら説明する。今交流電動機
は8極で、電機子巻線の接続は2xYとする。第1図は
しや断固を含む結線略図で、図において一点鎖線て囲ん
だ内部が電機子巻線で、全体を#1回路と#2回路との
二つに分け、#1回路に属する三相巻線の口出端子をU
、、V、、W、、#2回路に属するそれらをU。、V。
、W。とする。全巻線の電源側に#1しや断固を接続し
、#2回路のみの電源側に#2しや断固を接続する。始
動順序としてはまず#2しや断固を開いたま、の状態で
#1しや断固を投入する。すると電力は#1回路の電機
子巻線のみに供給され交流電動機は全巻線を使用した場
合の約112の始動電流、同じく約112の始動トルク
で始動する。適当速度に加速した時点て更に#2しや断
固を投入すると全巻線に電力が供給され交流電動機は完
全に1台分の始動電流、トルクで加速し全速に達し定速
運転には入る。第2図は第1図に示す交流電動機を軸方
向に見た電機子線輪の幾何学的配置を示す。尚第2図は
簡単のため#1回路U相のみ口出端子から中性点“’0
’’までの接続を示している。又内側の歯車状の図形は
回転子磁極を示し、電機子巻線との相対位置を明示する
ため描いてある。図から明らかなように#1回路に属す
る二つの線輪群、U相で言えば口出端子U1から接続さ
れた第1象限の1−U,l−(−U)の線輪群とそれら
から渡り線を介して接続された中性点゜“0゛に至る1
−U,l−(−U)の線輪群とが電機子鉄心上幾何学的
に正反対の位置に配置接続されているため、回転子を一
方のみに吸引する不平衡磁気吸引力は発生しない。従つ
て#1しや断器を投入し#1回路の線輪のみに電力を供
給して加速しても磁気的不平衡による異常は生じない。
回転子が加速をほぼ完了した時#2しや断器を投入し#
2回路に属する線輪に電力を供給しても#2回路に属す
る線輪も同様に各線輪群が幾何学的に対称の位置に配置
接続されているので不平衡は生じない。このような従来
の方法では電機子巻線の並列回路数をmとした場合、交
流電動機の極数が加の倍数でない場合には一つの回路に
属する二つの線輪群が相互に等しい極数を持ち得ないた
め、二群が対称に配置できず不平衡磁気吸引力を生じ始
動中過大な振動電流およびトルク脈動などの不具合を生
ずることである。このことを具体的に第3図を参照しな
がら説明する。図の電機子巻線配置は2XY接続、w極
の交流電動機の場合を示すものである。即ち並列回路数
mぱ゜2゛,従つて?の倍数は4,8,12,16,・
・であり、1巾は加の倍数では無い。しや断器を含む全
体接続は第1図と同じ、巻線配置接続の図示要領は第2
図と同様、但し回転子磁極の位置は略してある。第3図
に於て#1回路に属する二つの線輪群、U相で言えば口
.出端子U1に接続された第1象限の1−U,l一(−
U)の線輪群とそれから渡り線を通つて接続された中性
点゜“0゛に至る第3象限の1(一U),1−U,l−
(−U)の線輪群とは対称に配置てきない。換言すれば
#1回路に属する線輪.群は5極を構成しており、二群
に分ける場合等しい極数を持たせることはできない。第
3図では口出端子U,に近い線輪群が2極、中性点に近
い線輪群が3極を構成している。更に言えは第3図中“
×゛印を付した位置の線輪群の対称反対側の線・輪群は
“Δ゛印を付して示すが、#1回路に属さず#2回路に
属しているので、#1回路の線輪群に給電始動加速する
場合磁気的に不平衡になり前記の如き不具合を生じ分割
巻線始動方式を適用できない。従つて本発明は加の倍数
でない極数の交流電動機でも磁気的不平衡を生じさせな
いようにして任意の極数の場合でも自由に分割巻線始動
を採用できるようにした交流電動機を得ることを目的と
する。
These starting methods include reactor starting, condolfer starting, starting using a starter motor, and among these, split winding starting is a simple method that does not require special equipment and has good starting efficiency. Split-winding starting is a method in which the armature winding is divided into several parallel circuits, a part of which is used during starting, and the parallel circuits are activated as appropriate depending on acceleration. Many specific methods are known, but among them, two or more parallel circuits are provided in the armature winding of an AC motor with a relatively large number of poles, and the wires belonging to one circuit are There is a method of preventing magnetic imbalance during starting by dividing the rings into two groups based on their geometrical arrangement and arranging each group at diametrically opposite positions on the armature core. A more specific example will be described below with reference to the drawings. The AC motor has 8 poles, and the armature winding connections are 2xY. Figure 1 is a schematic diagram of the connection, including the connection. Connect the output terminal of the phase winding to U.
, ,V, ,W, ,U those belonging to the #2 circuit. ,V.
,W. shall be. Connect #1 Shiya-ketsu to the power supply side of all windings, and connect #2 Shiya-ketsu to the power supply side of only #2 circuit. As for the starting order, first leave #2 Shiya-ketsu open, then put in #1 Shiya-ketsu. Then, power is supplied only to the armature winding of the #1 circuit, and the AC motor starts with a starting current of about 112 and a starting torque of about 112 when all windings are used. When the engine accelerates to an appropriate speed, power is supplied to all windings and the AC motor is fully accelerated with the starting current and torque of one engine, reaching full speed and entering constant speed operation. FIG. 2 shows the geometrical arrangement of the armature coils when the AC motor shown in FIG. 1 is viewed in the axial direction. For simplicity, Figure 2 shows only the #1 circuit U phase from the output terminal to the neutral point "'0".
'' shows connections up to. The inner gear-shaped figure indicates the rotor magnetic pole, and is drawn to clearly indicate the relative position with the armature winding. As is clear from the figure, there are two wire groups belonging to the #1 circuit, in terms of the U phase, the wire groups 1-U and l-(-U) in the first quadrant connected from the output terminal U1 and their 1 to the neutral point ゜“0゛” connected via a crossover wire.
-U, l- (-U) wire rings are arranged and connected at geometrically opposite positions on the armature core, so an unbalanced magnetic attraction force that attracts the rotor to only one side is not generated. . Therefore, even if the #1 circuit breaker is turned on and power is supplied to only the coils of the #1 circuit for acceleration, no abnormality will occur due to magnetic imbalance.
When the rotor has almost completed its acceleration, turn on the #2 breaker.
Even if power is supplied to the coils belonging to the #2 circuit, no unbalance will occur since the coil groups belonging to the #2 circuit are arranged and connected in geometrically symmetrical positions. In this conventional method, when the number of parallel circuits of the armature winding is m, if the number of poles of the AC motor is not an additive multiple, the two wire ring groups belonging to one circuit have the same number of poles. Therefore, the two groups cannot be arranged symmetrically, resulting in an unbalanced magnetic attraction force, resulting in problems such as excessive oscillating current and torque pulsation during startup. This will be specifically explained with reference to FIG. The armature winding arrangement shown in the figure is for a 2XY connection, w-pole AC motor. That is, the number of parallel circuits m is 2゛, so ? The multiples of are 4, 8, 12, 16,・
・And one width is not a multiple of addition. The overall connection including the shield and disconnector is the same as in Figure 1, and the drawing instructions for winding arrangement and connection are as in Figure 2.
Similar to the figure, however, the positions of the rotor magnetic poles are omitted. In Fig. 3, there are two wire ring groups belonging to the #1 circuit, in terms of the U phase. 1-U, l-(-
1 (1U), 1-U, l- of the third quadrant leading to the neutral point ゛0゛ connected to the line ring group of U) and the wire through the connecting wire.
It cannot be arranged symmetrically with the line ring group (-U). In other words, the wires belong to the #1 circuit. The group consists of five poles, and when divided into two groups, it is not possible to have the same number of poles. In FIG. 3, the wire ring group near the outlet terminal U constitutes two poles, and the wire ring group near the neutral point constitutes three poles. Furthermore, in Figure 3 “
The line/ring group on the symmetrical side of the line/ring group at the position marked with ×゛ is marked with “∆”, but it does not belong to #1 circuit but belongs to #2 circuit, so it is connected to #1 circuit. When starting and accelerating the power supply to a group of wire wheels, magnetic imbalance occurs and the above-mentioned problems occur, making it impossible to apply the split winding starting method.Therefore, the present invention can solve the problem of magnetic imbalance even in AC motors with a pole number that is not a multiple of the sum. An object of the present invention is to obtain an AC motor in which split winding starting can be freely adopted even in the case of an arbitrary number of poles without causing equilibrium.

以下本発明による交流電動機の一実施例について図面を
参照しながら詳細に説明する。
An embodiment of the AC motor according to the present invention will be described in detail below with reference to the drawings.

第4図は第3図と同じく2XY接続m極の交流電動機の
電機ノ子巻線配置接続図てあるが、本発明を適用してあ
る。即ち図において相対向するΔ印および×印の位置に
ある極に属する各相の線輪群を各々2分し、2分された
各線輪小群を各各別の回路即ち#1と#2の回路にそれ
ぞれ属するよう接続す.る。即ち#1回路と#2回路と
の間で線輪小群が交換された形にする。このように接続
して第1図に示す#1しや断器を投入し#1回路の電機
子巻線に電力を供給すると第3図に示す従来の巻線接続
では磁気的不平衡の原因となつていた×印で示・す位置
の極の線輪群は半分の小群のみが励磁され、それと反対
側て従来励磁されなかつたΔ印て示す位置の極の線輪群
は新らたに半分の小群が励磁されるので、第4図の×印
の極とΔ印の極とは磁気的にほぼ平衡した励磁状態とな
り、磁気的不平衡はほぼ消滅する。尚完全には消滅しな
い理由は後述する。次に#2しや断器を投入し#2回路
の電機子巻線にも電力を供給するとこの交流電動機の全
巻線が付勢され磁気的不平衡は全く無くなり、加速して
全速に達し普通の2XY接続の交流電動機と変らない特
性で運転する。次に第4図で概念的に示されているΔ印
、×印の極に属する線輪群の分割方法について詳細に説
明し、あわせて前記した磁気的不平衡を完全には消滅さ
せ得ない理由を説明する。
FIG. 4 is a diagram showing the arrangement and connection of the armature windings of a 2XY-connected m-pole AC motor, similar to FIG. 3, but to which the present invention is applied. In other words, the coil groups of each phase belonging to the poles located at the opposite positions of Δ and Connect them so that they belong to the respective circuits. Ru. That is, the small group of coils is exchanged between the #1 circuit and the #2 circuit. When connected in this way and the #1 circuit breaker shown in Figure 1 is turned on to supply power to the armature winding of the #1 circuit, the conventional winding connection shown in Figure 3 causes magnetic unbalance. Only half of the small group of wire rings at the poles at the positions indicated by the × marks are excited, and on the other side, the wire ring groups at the poles at the positions indicated by the Δ marks, which were not previously excited, are now being energized. Since only half of the small groups are excited, the poles marked with x and the poles marked with Δ in FIG. 4 are in an almost magnetically balanced excitation state, and the magnetic unbalance almost disappears. The reason why it does not disappear completely will be explained later. Next, when the #2 circuit breaker is turned on and power is also supplied to the armature winding of the #2 circuit, all the windings of this AC motor are energized, the magnetic unbalance disappears, and it accelerates to full speed. It operates with the same characteristics as a 2XY connection AC motor. Next, we will explain in detail the method of dividing the line ring groups belonging to the poles marked Δ and Explain why.

第4図てはUl,U2:■1,■2:Wl,W2各相の
端子が各々電源側側R,S,T各相に接続された時、時
計方向(右回転)の回転磁界を生ずるように線輪が配置
接続されている。今U相の#1回路のΔ印,×印の線輪
小群について見るとΔ印側では磁界の回転方向に対して
一つの相帯内で線輪が空間的に遅れ側の位置を占め、反
対側×印側では逆に一つの相帯内て線輪が空間的には進
み側の位置を占めている。同様にU相の#2回路を見て
みると#1回路と逆にΔ印側で進み、×印側で遅れの線
輪配置となつている。従つて#1回路、#2回路共に遅
れ位置の線輪小群と進み位置の線輪小群とを含んでいる
のて両回路の誘起電圧の位相は一致し両回路間に循環電
流は流れない。しかしこの位置では第4図で明らかなよ
うに一つの回路で2ケの線輪小群は電機子上ほぼ反対側
に位置しているが正反対位置では無い。従つてわずかな
磁気的不平衡が残ることになるが、前述の如く両回路間
に循環電流を流さないようにするため止むを得ない。但
し、第4図てはW相の線輪小群を#1回路と#2回路に
割りふる順序を他のU,■相の場合と逆にしてある。こ
のようにすると三相共同じ順序で割りふつた場合より磁
気的不平衡は更に低減される。更に線輪小群を構成する
時に#1回路,#2回路に交互に線輪を割りふるように
すれば一層磁気不平衡低減効果がある。尚、一極一相の
線輪群を小群に分割する時各小群がなるべく同数の線輪
数となることが望ましいが、一極一相の線輪数が奇数の
場合は同数にできないので偶数の場合よりも残留する磁
気的不平衡が大きくなる。この場合、第4図て△印側て
#1回路のU,V相の小群の線輪数を大にし、−W相の
小群の線輪数を小にすると同時に反対側の×印側では#
1回路の−U,−■相の線輪小群の線輪数を小とし、W
相の小群の線輪数を大とすると一層磁気的不平衡低減効
果かある。以上記載の本発明によれば毎極毎相の線輪群
の分割および接続を簡単容易に変えるだけで任意の極数
の場合でも外部的には全く変らない回路で分割巻線始動
を採用できる交流電動機が得られ、分割巻線始動方式採
用についての極数の制約が無くなる大きな利点が得られ
る。
In Figure 4, when the terminals of each phase of Ul, U2: ■1, ■2: Wl, W2 are connected to the R, S, and T phases on the power supply side, a clockwise (clockwise rotation) rotating magnetic field is generated. The wire rings are arranged and connected so as to occur. Now, looking at the wire ring small groups marked with Δ and × in the #1 circuit of the U phase, on the side marked with Δ, the wire rings spatially occupy a position on the lagging side within one phase zone with respect to the rotation direction of the magnetic field. On the other hand, on the opposite side marked with an x, the line ring within one phase zone spatially occupies a position on the advancing side. Similarly, if we look at the U-phase #2 circuit, it has a wire arrangement in which, contrary to the #1 circuit, it advances on the Δ side and lags on the × side. Therefore, since both the #1 circuit and the #2 circuit include a small group of wire wheels in a lagging position and a small group of wire wheels in an advanced position, the phases of the induced voltages in both circuits match, and a circulating current flows between both circuits. do not have. However, in this position, as is clear from FIG. 4, the two wire ring groups in one circuit are located on almost opposite sides of the armature, but not in exactly opposite positions. Therefore, a slight magnetic imbalance will remain, but this is unavoidable in order to prevent circulating current from flowing between the two circuits as described above. However, in FIG. 4, the order of allocating the W-phase wire ring small group to the #1 circuit and #2 circuit is reversed from that for the other U and ■ phases. In this way, magnetic unbalance is further reduced than when all three phases are divided in the same order. Furthermore, when forming a small group of coils, if the coils are allocated alternately to the #1 circuit and the #2 circuit, the magnetic unbalance can be further reduced. When dividing a single-pole, single-phase wire ring group into small groups, it is desirable that each small group have the same number of wire wheels as possible, but if the number of wire wheels on a single pole and one phase is an odd number, it is not possible to make them the same number. Therefore, the residual magnetic unbalance becomes larger than in the case of an even number. In this case, increase the number of wires in the U and V phase small group of #1 circuit on the side marked with △ in Figure 4, and decrease the number of wires on the small group of -W phase at the same time on the side marked with × on the opposite side. On the side #
The number of wires in the -U, -■ phase wire ring small group of one circuit is small, and W
Increasing the number of wires in a small group of phases has the effect of further reducing magnetic imbalance. According to the present invention described above, by simply and easily changing the division and connection of the coil group for each pole and each phase, split winding starting can be adopted with a circuit that does not change externally at all even in the case of any number of poles. An AC motor is obtained, and there is a great advantage that there is no restriction on the number of poles when adopting the split winding starting method.

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

第1図は分割巻線始動方式の結線路図、第2図は8極の
交流電動機を軸方向より見た電機子巻線配置接続図、第
3図は1師の交流電動機を軸方向より見た電機子巻線配
置接続図、第4図は本発明による1晰の交流電動機を軸
方向より見た電機子線輪配置接続図てある。 1・・・・・・#1回線に属するコイル群、2・・・・
・・#2回線に属するコイル群。
Figure 1 is a connection diagram of a split winding starting method, Figure 2 is an armature winding arrangement and connection diagram of an 8-pole AC motor viewed from the axial direction, and Figure 3 is a connection diagram of a single-pole AC motor viewed from the axial direction. FIG. 4 is a diagram showing the arrangement and connection of armature windings as seen from the axial direction of a one-lucid AC motor according to the present invention. 1... Coil group belonging to #1 line, 2...
...Coil group belonging to #2 line.

Claims (1)

【特許請求の範囲】[Claims] 1 電機子巻線各相に2個以上の並列回路を設けて分割
巻線始動を行なう場合、その並列回路数の2倍で割り切
れない極数の時生ずる軸心に関して相対向する二つの極
の下で異なる並列回路に属する毎極毎相の線輪群をそれ
ぞれ分割し、分割された線輪又は線輪小群を両方の極の
下ともそれぞれの並列回路に属する如く接続し、同じ並
列回路に属する線輪又は線輪小群が相対向する極位置に
それぞれ配置される如くにした電機子巻線を備えた多相
交流電動機。
1. When performing split winding starting by installing two or more parallel circuits in each phase of the armature winding, two poles facing each other with respect to the axis occur when the number of poles is not divisible by twice the number of parallel circuits. Below, the wire groups of each pole and each phase belonging to different parallel circuits are divided, and the divided wire rings or wire ring subgroups are connected under both poles as if they belong to each parallel circuit, and the same parallel circuit is connected. A polyphase AC motor equipped with an armature winding in which wire rings or small groups of wire rings belonging to the above are arranged at opposite pole positions.
JP8015777A 1977-07-05 1977-07-05 polyphase alternating current motor Expired JPS6048985B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8015777A JPS6048985B2 (en) 1977-07-05 1977-07-05 polyphase alternating current motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8015777A JPS6048985B2 (en) 1977-07-05 1977-07-05 polyphase alternating current motor

Publications (2)

Publication Number Publication Date
JPS5415112A JPS5415112A (en) 1979-02-03
JPS6048985B2 true JPS6048985B2 (en) 1985-10-30

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP8015777A Expired JPS6048985B2 (en) 1977-07-05 1977-07-05 polyphase alternating current motor

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JP (1) JPS6048985B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59195232U (en) * 1983-06-14 1984-12-25 日本発条株式会社 spring clutch
JP4665595B2 (en) * 2005-04-28 2011-04-06 トヨタ自動車株式会社 Winding structure of rotating electrical machine

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Publication number Publication date
JPS5415112A (en) 1979-02-03

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