JPH0221216B2 - - Google Patents

Info

Publication number
JPH0221216B2
JPH0221216B2 JP55059072A JP5907280A JPH0221216B2 JP H0221216 B2 JPH0221216 B2 JP H0221216B2 JP 55059072 A JP55059072 A JP 55059072A JP 5907280 A JP5907280 A JP 5907280A JP H0221216 B2 JPH0221216 B2 JP H0221216B2
Authority
JP
Japan
Prior art keywords
load
electromagnetic coupling
rotor
stator
electromagnetic
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 - Lifetime
Application number
JP55059072A
Other languages
Japanese (ja)
Other versions
JPS56156420A (en
Inventor
Fukuo Shibata
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP5907280A priority Critical patent/JPS56156420A/en
Publication of JPS56156420A publication Critical patent/JPS56156420A/en
Publication of JPH0221216B2 publication Critical patent/JPH0221216B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Dynamo-Electric Clutches, Dynamo-Electric Brakes (AREA)

Description

【発明の詳細な説明】 電磁継手と固定子を持つた回転電気機械の機械
的且つ電気的結合によつて原動機より負荷へ動力
を伝達する装置が既に昭和53年特許出願公告第62
号や特許出願公開昭53−35848号に示されている。
これらの装置では機械的歯車装置を用いないで、
動力伝達減速機構を造りうるので、信頼性が高
く、トルク変動の大きいデイーゼル機関から減速
して負荷を駆動するような動力伝達装置には適し
ているように思われる。然しこのような従来の動
力伝達装置にも大きい欠点がある。それは負荷の
回転速度が低い場合、電磁継手と結合する回転電
気機械の寸法が非常に大きくなることにより不経
済な装置になるだけではなく、効率が悪くなると
云う欠点である。殊に回転電気機械が誘導電動機
のような場合、負荷側の回転速度が特に低く
50rpmなどとなれば容量の大きい誘導電動機、例
えば5000KWのようなものは製作不可能又は製作
困難であり、効率も極めて悪い。
[Detailed Description of the Invention] A device for transmitting power from a prime mover to a load by mechanically and electrically coupling a rotating electrical machine having an electromagnetic coupling and a stator has already been disclosed in Patent Application Publication No. 62 in 1982.
No. 53-35848.
These devices do not use mechanical gearing;
Since it is possible to create a power transmission reduction mechanism, it is highly reliable and seems suitable for a power transmission device that drives a load by decelerating a diesel engine with large torque fluctuations. However, such conventional power transmission devices also have major drawbacks. The disadvantage is that when the rotational speed of the load is low, the dimensions of the rotating electric machine connected to the electromagnetic coupling become very large, which not only makes the device uneconomical, but also reduces its efficiency. Especially when the rotating electric machine is an induction motor, the rotation speed on the load side is particularly low.
If the speed is 50 rpm, it is impossible or difficult to manufacture a large-capacity induction motor, such as 5000 KW, and the efficiency is extremely low.

今船舶の推進を例に考える。エネルギーの節約
のため、船舶推進機関の主力はデイーゼル機関に
なつたが、デイーゼル機関には400rpm程度の4
サイクル機関と100rpm程度の2サイクル機関が
現在の大容量デイーゼル機関の二種類としてあげ
られる。このようなデイーゼル機関により駆動さ
れる船舶のプロペラ回転速度はその船舶推進効率
を上げるため、従来100rpm程度であつたのを
50rpm程度に下げることが最近の傾向である。こ
のような場合に前述の特許出願公告昭和53年第62
号や特許出願公開昭53−第35848号に示された従
来の電磁的動力伝達装置では前記の不都合を生じ
る。従来公知のこの特許出願公開昭53−35848号
の場合、前述のように電磁継手と電気的且つ機械
的に結合した固定子を持つ回転電気機械の寸法が
大きくなる欠点があるが、それよりも固定子を持
つ回転電気機械の軸方向の長さが長いため、特許
出願公開昭53−35848号に示した配列のように電
磁継手と負荷の間に固定子式回転電気機械を挿入
配列した場合、原動機と負荷の間の動力伝達装置
全体の長さが長くなる。そこで船舶の機関室の長
さを長くせざるを得ないと云うように、配置上の
不都合を生じる結果にもなる。
Let's take ship propulsion as an example. In order to save energy, the main power of marine propulsion engines has become diesel engines, but diesel engines have a speed of about 400 rpm.
Cycle engines and 100rpm two-cycle engines are the two types of current large-capacity diesel engines. The propeller rotation speed of ships driven by such diesel engines has been increased from about 100 rpm in the past in order to increase the ship's propulsion efficiency.
The recent trend is to lower the speed to about 50 rpm. In such a case, the above-mentioned patent application publication No. 62 of 1978
The conventional electromagnetic power transmission device disclosed in Japanese Patent Application No. 53-35848 has the above-mentioned disadvantages. In the case of this conventionally known patent application No. 1983-35848, as mentioned above, there is a disadvantage that the size of the rotating electric machine having the stator electrically and mechanically coupled to the electromagnetic coupling becomes large. Since the axial length of a rotating electric machine with a stator is long, when a stator type rotating electric machine is inserted between the electromagnetic joint and the load as shown in the arrangement shown in Patent Application Publication No. 53-35848. , the length of the entire power transmission device between the prime mover and the load becomes longer. This also results in inconveniences in layout, such as having to lengthen the engine room of the ship.

一方、特許出願公開昭53−35848号において突
発的負荷変動を生じたような場合、乱調を生じる
可能性がある。すなわち固定子を持つ回転電気機
械が同期電動機の場合を例にとつて考えると、一
定の負荷では同期電動機の負荷角δ1及び電磁継手
の負荷角δ2が共に一定の状態で運転するが、負荷
が変化すると同期電動機の負荷角δ1も電磁継手の
負荷角δ2も共に変化する。今負荷が急に増すと、
同期電動機の負荷角δ1が増すが、同期電動機の負
荷角δ1の増加はそれ自身だけで増加するのではな
く、電磁継手の負荷角δ2の増加する結果となるの
である。この場合の電磁継手の負荷角δ2は電磁継
手を同期電動機と考えた場合の負荷角δ2である。
すなわち電磁継手は原動機側の回転速度と負荷側
の回転子の回転速度との間の速度差を回転速度と
した同期電動機と考えた場合の無負荷誘導起電力
と端子電圧との間の位相差を負荷角と考えるので
ある。
On the other hand, if a sudden load change occurs, as in Patent Application Publication No. 53-35848, there is a possibility that disturbances may occur. In other words, if we consider the case where the rotating electric machine with a stator is a synchronous motor, at a constant load, the synchronous motor operates with both the load angle δ 1 and the electromagnetic coupling load angle δ 2 constant. When the load changes, both the load angle δ 1 of the synchronous motor and the load angle δ 2 of the electromagnetic joint change. If the load suddenly increases,
The load angle δ 1 of the synchronous motor increases, but the increase in the load angle δ 1 of the synchronous motor does not increase by itself, but results in an increase in the load angle δ 2 of the electromagnetic joint. The load angle δ 2 of the electromagnetic joint in this case is the load angle δ 2 when the electromagnetic joint is considered as a synchronous motor.
In other words, the phase difference between the no-load induced electromotive force and the terminal voltage when an electromagnetic coupling is considered to be a synchronous motor whose rotation speed is the speed difference between the rotation speed of the prime mover side and the rotation speed of the rotor on the load side. is considered to be the load angle.

今同期電動機と結合した電磁継手の負荷が急に
過負荷となる場合を考える。その場合、同期電動
機の負荷角がδ1より増す時、同期電動機としての
電磁継手の負荷角δ2も第3図のように増す。この
ように負荷が急激に過負荷状態になると、同期電
動機及び同期発電機としての電磁継手の負荷角が
増そうとするが、新負荷に応じる新負荷角に直ち
に落ち付かず、回転体の慣性のために、その点を
中心に負荷角の周期的変動をくり返す。このよう
な乱調現象を生じ、不安定な運転状態となる。乱
調が甚はだしくなり、負荷角の変動範囲が大きく
なると、遂に同期期電動機は電源との同期を脱出
して停止するようになり、同期発電機としての電
磁継手も同期の脱出により停止するようになる。
第3図ではそのような負荷角の変動範囲の限界域
をδ3で表わし、それ以上の負荷角になると、上記
の脱出状態になることが示される。
Now consider the case where the load on the electromagnetic joint connected to the synchronous motor suddenly becomes overloaded. In that case, when the load angle of the synchronous motor increases from δ 1 , the load angle δ 2 of the electromagnetic joint as a synchronous motor also increases as shown in FIG. When the load suddenly becomes overloaded in this way, the load angle of the electromagnetic coupling as a synchronous motor and synchronous generator tries to increase, but it does not immediately settle to the new load angle corresponding to the new load, and the inertia of the rotating body increases. Therefore, the load angle is periodically varied around that point. Such a disturbance phenomenon occurs, resulting in an unstable operating state. When the disturbance becomes severe and the variation range of the load angle becomes large, the synchronous motor finally loses synchronization with the power supply and stops, and the electromagnetic coupling as a synchronous generator also stops due to the loss of synchronization. It becomes like this.
In FIG. 3, the limit range of such a variation range of the load angle is represented by δ 3 , and it is shown that when the load angle exceeds this range, the above-mentioned escape state occurs.

本発明の目的は電磁継手と固定子を持つ回転電
気機械の電気的且つ機械的結合による動力伝達装
置において以上述べた公知の特許出願公告昭和53
年第62号や特許出願公開昭53−35848号の欠点を
除き、固定子を持つ回転電気機械の寸法重量を小
形化し、且つその動力伝達装置の長さ方向の寸法
を短かくし、それにより配列を短縮すると共に、
他方、負荷の急変時に乱調から脱出に到るのを防
ぎ、動力伝達装置の過渡的安定度を高めることに
ある。
The object of the present invention is to provide a power transmission device based on electrical and mechanical coupling of a rotating electric machine having an electromagnetic coupling and a stator, which is based on the above-mentioned known patent application publication.
No. 62 of 2013 and Patent Application Publication No. 53-35848, it is possible to reduce the size and weight of a rotating electric machine having a stator, shorten the longitudinal dimension of its power transmission device, and thereby improve the alignment. In addition to shortening the
On the other hand, the purpose is to prevent the system from going out of control when the load suddenly changes, and to improve the transient stability of the power transmission device.

以上の号的を達成せしめるため、本発明では第
1図の具体的接続図例と第2図の部分構成図例に
示すように、相対的に回転し、相対向する二つの
回転子1と2を有し、少なくともその一方の回転
子1に電機子巻線22を有する電磁継手18の負
荷側回転子1と大歯車9を結合し、一方固定子を
持つ回転電気機械7の回転子と結合した小歯車1
0を上記大歯車9とかみ合わせて減速歯車装置8
を造ることにより、上記固定子を持つ回転電気機
械7の回転子の出力軸17から上記減速歯車装置
8を経て負荷6へ減速動力伝達しうるように配列
し、一方電磁継手18の負荷側回転子1により直
接負荷6を駆動すべく、電磁継手18の負荷側回
転子1と負荷6の間を機械的に結合すると共に、
この電磁継手18の他方の回転子2を原動機5で
回転駆動せしめるように配列し、而も上記固定子
を持つ回転電気機械7と上記電磁継手18の電機
子巻線間を電気接続することによつて上記固定子
を持つ回転電気機械7が電磁継手18の電気出力
端子より電力を受けるように配列し、原動機5の
出力軸11からの出力を電磁継手18を経て、一
方は直接に機械力として負荷6を駆動し、他方は
電磁継手18の電気出力としてこれを固定子を持
つ回転電気機械7へ興え、それから変換された機
械出力を上記減速歯車装置8を経て負荷6へ動力
伝達するように配列し、上記電磁継手18の回転
子2の界磁極23の極表面に制動巻線21を設
け、籠形誘導機の回転子巻線のように制動巻線2
1相互間を短絡することを特長とするのである。
In order to achieve the above objectives, the present invention has two rotors 1 that rotate relatively and face each other, as shown in the specific connection diagram example in FIG. 1 and the partial configuration diagram example in FIG. 2. 2, the load-side rotor 1 of an electromagnetic coupling 18 having an armature winding 22 on at least one of the rotors 1 and the large gear 9 are coupled, and the rotor of a rotating electric machine 7 having a stator on the other hand Combined small gear 1
0 is meshed with the large gear 9 to form a reduction gear device 8.
is arranged so that deceleration power can be transmitted from the output shaft 17 of the rotor of the rotary electric machine 7 having the stator to the load 6 via the reduction gear device 8, while the load side rotation of the electromagnetic coupling 18 is In order to directly drive the load 6 by the child 1, the load side rotor 1 of the electromagnetic coupling 18 and the load 6 are mechanically coupled, and
The other rotor 2 of this electromagnetic coupling 18 is arranged so as to be rotationally driven by the prime mover 5, and electrical connection is made between the rotating electrical machine 7 having the stator and the armature winding of the electromagnetic coupling 18. Therefore, the rotating electric machine 7 having the stator is arranged so as to receive electric power from the electric output terminal of the electromagnetic coupling 18, and one side directly receives the mechanical power from the output shaft 11 of the prime mover 5 through the electromagnetic coupling 18. The other drives the load 6 as the electric output of the electromagnetic coupling 18 to the rotary electric machine 7 having a stator, and then transmits the converted mechanical output to the load 6 via the reduction gear device 8. The brake winding 21 is arranged on the pole surface of the field pole 23 of the rotor 2 of the electromagnetic coupling 18, and the brake winding 21 is arranged like the rotor winding of a cage induction machine.
It is characterized by shorting between the two.

以上の電磁継手18の場合、回転子1と2の
中、回転子1に電機子巻線22を設け、その電機
子巻線22と外部機器との接続のためにスリツプ
リング3を設け、回転電気機械7の電機子巻線と
の間の電気接続は電線14でおこなう。回転子1
と云うのは負荷6との間で軸12によつて結合さ
れる回転子を示すものであつて、電機子巻線が原
動機5を出力軸11と結合される回転子2に設け
られる場合も考えられる。歯車装置8は電磁継手
18の回転子中、負荷6と結合される回転子1と
結合される。第1図の場合、歯車装置8はピニオ
ン10と大歯車9とより成る一段式であり、回転
電気機械7の出力軸17から負荷6の方へ見て歯
車装置8は一段減速となる。図では電磁継手18
の回転子2に直流励磁電流が供給される界磁巻線
20が設けられるが、その外部接続のための端子
としてスリツプリング4が設けられ、定常運転時
にはその電機子巻線22からスリツプリング3、
交流電気接続電線15、整流器13、直流電気接
続電線16を経てスリツプリング4へ励磁電流が
供給される。然し、必らずしも界磁巻線用の励磁
電流をそのような自励式に供給する必要はなく、
他の直流電源からも供給しうる。特に始動時には
そのような他励方式とすることもある。回転電気
機械7は同期電動機でもよく、籠形誘導電動機で
も良い。負荷6の回転速度が50rpmであり、歯車
装置8の減速比が8であるとすれば、回転電気機
械7の回転速度を400rpmとなしうるので、
50rpmの場合にくらべると、かなり製作しやすく
なるし、又安価にもなる。更に効率も良くなる。
例えば籠形誘導電動機5000KW出力で50rpmの回
転速度の定格の効率を90%とするならば、
5000KW,400rpmのそれを94%とすることが出
来、歯車装置の効率をそこで99.2%とすると、総
合効率は93%程度となり、明らかに3%程度の向
上を期しうることになる。この歯車装置を二段結
合とし、例えば36対1の減速を得るとすれば、回
転電気機械7の回転速度を1800rpmとし、回転電
気機械7の大きさを更にコンパクトにし、効率を
更に上げることが出来る。回転電気機械7の効率
をその場合98%にすることは容易であるし、歯車
装置の効率を98.5%とすると、総合効率は96%と
なる。回転電気機械7として巻線形誘導電動機を
用い、その一次又は二次回路に周波数変換装置を
接続することも出来る。第1図で電気接続線14
の回路に正逆の相順変換開閉装置を設け、相の接
続を正方向にも逆方向にもなるように配列しう
る。それにより原動機5の回転方向と負荷6の回
転方向を互いに同方向とすることも出来るし、相
互に逆方向にすることも出来る。
In the case of the electromagnetic coupling 18 described above, the armature winding 22 is provided on the rotor 1 among the rotors 1 and 2, and the slip ring 3 is provided to connect the armature winding 22 with external equipment. The electrical connection with the armature winding of the electric machine 7 is made by electric wires 14. Rotor 1
This refers to a rotor that is connected to the load 6 by the shaft 12, and also when the armature winding is provided on the rotor 2 that connects the prime mover 5 to the output shaft 11. Conceivable. The gear system 8 is connected to the rotor 1 of the electromagnetic coupling 18 , which is connected to the load 6 . In the case of FIG. 1, the gear device 8 is a one-stage type consisting of a pinion 10 and a large gear 9, and the gear device 8 has a one-stage reduction when viewed from the output shaft 17 of the rotating electrical machine 7 toward the load 6. In the figure, electromagnetic joint 18
A field winding 20 is provided to which DC excitation current is supplied to the rotor 2, and a slip ring 4 is provided as a terminal for external connection of the field winding 20, and during steady operation, the armature winding 22 is connected to the slip ring 3. ,
Excitation current is supplied to the slip ring 4 via an AC electrical connection wire 15, a rectifier 13, and a DC electrical connection wire 16. However, it is not necessarily necessary to supply the excitation current for the field winding in such a self-excited manner;
It can also be supplied from other DC power sources. Particularly during startup, such a separately excited system may be used. The rotating electric machine 7 may be a synchronous motor or a cage induction motor. If the rotation speed of the load 6 is 50 rpm and the reduction ratio of the gear device 8 is 8, then the rotation speed of the rotating electric machine 7 can be set to 400 rpm.
Compared to the case of 50 rpm, it is much easier to manufacture and also cheaper. It also improves efficiency.
For example, if the rated efficiency of a cage induction motor with a 5000KW output and a rotation speed of 50rpm is 90%,
If the efficiency of 5000KW and 400rpm can be made 94%, and the efficiency of the gear device is 99.2%, the overall efficiency will be about 93%, which clearly means that an improvement of about 3% can be expected. If this gear device is a two-stage combination and a reduction ratio of, for example, 36:1 is obtained, the rotational speed of the rotating electric machine 7 is set to 1800 rpm, the size of the rotating electric machine 7 is made more compact, and the efficiency is further increased. I can do it. In that case, it is easy to make the efficiency of the rotating electric machine 7 98%, and if the efficiency of the gear device is 98.5%, the overall efficiency is 96%. It is also possible to use a wound induction motor as the rotating electrical machine 7 and connect a frequency converter to its primary or secondary circuit. Electrical connection line 14 in Figure 1
A forward/reverse phase conversion switchgear is provided in the circuit, and the phase connections can be arranged in either the forward direction or the reverse direction. Thereby, the rotation direction of the prime mover 5 and the rotation direction of the load 6 can be made to be the same direction or to be made to be in opposite directions.

回転電気機械7を直流機とし、その電機子巻線
と電磁継手18の電機子巻線との間を整流器を経
て電気接続することも出来る。回転電気機械7を
無整流子電動機とすることも出来る。
It is also possible to use a DC machine as the rotating electric machine 7 and electrically connect its armature winding to the armature winding of the electromagnetic joint 18 via a rectifier. The rotating electrical machine 7 can also be a commutatorless motor.

本発明の動作を説明する。原動機5によつて電
磁継手18の一方の回転子2を回転速度n0rpmで
駆動すると、他方の回転子1はn2rpmcm2回転し、
n0−n2なる速度差n1により電磁継手18は発電電
力をスリツプリング3の外部へ出し、その電力を
回転電気機械7が受ける。第1図では回転子1の
電機子巻線22に電流が流れ、回転子2の界磁極
23との間で電磁継手の作用が成立ち、原動機5
の回転速度n0の中のn2分だけ直接負荷6の方に軸
12を通し、電磁継手18の負荷側回転子1から
トルクが伝達され、n1分が電磁継手18より回転
電気機械7へ電力供給される。
The operation of the present invention will be explained. When one rotor 2 of the electromagnetic coupling 18 is driven by the prime mover 5 at a rotational speed n 0 rpm, the other rotor 1 rotates n 2 rpm cm 2 ,
Due to the speed difference n 1 of n 0 -n 2 , the electromagnetic coupling 18 outputs the generated power to the outside of the slip ring 3, and the rotating electrical machine 7 receives the power. In FIG. 1, current flows through the armature winding 22 of the rotor 1, and an electromagnetic coupling effect is established between it and the field pole 23 of the rotor 2, and the motor 5
The shaft 12 passes directly to the load 6 for n 2 minutes out of the rotational speed n 0 , and torque is transmitted from the load side rotor 1 of the electromagnetic coupling 18, and for n 1 minute, the torque is transmitted from the electromagnetic coupling 18 to the rotating electrical machine 7. Power is supplied to the

いま、回転電気機械7を同期電動機とすれば、
次の関係が成立つ。
Now, if the rotating electric machine 7 is a synchronous motor,
The following relationship holds true.

n1=n0−n2 (1) 120f=p1n1 (2) n2=n3/r (3) n3p2=120f (4) たゞし、fは電気接続線14における交流電力
の周波数、p1,p2はそれぞれ電磁継手18及び回
転電気機械7の極数、n3は回転電気機械7の回転
速度、rは歯車8の減速比である。
n 1 = n 0 − n 2 (1) 120f = p 1 n 1 (2) n 2 = n 3 /r (3) n 3 p 2 = 120f (4) The frequency of the AC power, p 1 and p 2 are the numbers of poles of the electromagnetic coupling 18 and the rotating electrical machine 7, respectively, n 3 is the rotational speed of the rotating electrical machine 7, and r is the reduction ratio of the gear 8.

(3)式を(4)式に代入して(2)式と比較すると、n2×
r×p2=p1n1となり、 n1=n2×r×p2/p1 (5) (1)式と(5)式より n0=n2(r×p2/p1+1) (6) 電気接続線14で電磁継手18と回転電気機械
7の両電機子巻線間を逆相順に接続すると、原動
機5の回転方向と負荷6の回転方向が互いに逆方
向となり、(1)式はn1=n0+n2となつて、(6)式はn0
=n2(r×p2/p1−1)となる。
Substituting equation (3) into equation (4) and comparing it with equation (2), we get n 2 ×
r x p 2 = p 1 n 1 , n 1 = n 2 x r x p 2 / p 1 (5) From equations (1) and (5), n 0 = n 2 (r x p 2 / p 1 +1) (6) When the electromagnetic coupling 18 and both armature windings of the rotating electrical machine 7 are connected in reverse phase order using the electrical connection wire 14, the rotation direction of the prime mover 5 and the rotation direction of the load 6 become opposite to each other, and ( Equation 1) becomes n 1 = n 0 + n 2 , and equation (6) becomes n 0
= n 2 (r×p 2 /p 1 −1).

いま第1図で原動機5の回転速度を100rpm、
負荷6の回転速度を50rpmとすると、上記(6)式に
おいてr=8、p1=32、p2=4とすれば成立つ。
すなわち低速原動機5から低速負荷6へ動力伝達
する場合、電磁継手18だけを多極機にして、回
転電気機械7を少極機として造りやすく、安価高
効率機となしうる。
Now, in Figure 1, the rotation speed of prime mover 5 is 100 rpm,
Assuming that the rotational speed of the load 6 is 50 rpm, the equation (6) above holds true if r=8, p 1 =32, and p 2 =4.
That is, when power is transmitted from the low-speed prime mover 5 to the low-speed load 6, only the electromagnetic coupling 18 is made into a multi-pole machine, and the rotating electric machine 7 can be easily manufactured as a small-pole machine, resulting in an inexpensive and highly efficient machine.

この場合、重要なことは例えばデイーゼル機関
のような原動機5から負荷のプロペラ6へ動力伝
達する時、その動力伝達機構の中に機械式歯車装
置を設けることはトルク変動を歯面に受けて信頼
性上好ましくないと考えられるのが一般的であ
る。然し本発明では電磁継手18の負荷側に歯車
装置8が接続されるので、原動機5の出力軸11
におけるトルク変動は電磁継手18に充分吸収さ
れ、歯車装置8へは伝達されない。つまり電磁継
手18は単に減速的機構を持つだけではなく、歯
車装置8の保護装置にもなるのである。そしてこ
の歯車装置8の容量は回転電気機械7のそれに対
応し、原動機5の容量のn1/n0分で良い。例え
ば、1万KWの原動機出力を動力伝達するとき、
原動機出力軸11の回転速度を100rpm,負荷6
の回転速度を50rpmとすれば、歯車装置8の容量
は5千KWで良い。
In this case, the important thing is that when power is transmitted from a prime mover 5 such as a diesel engine to a load propeller 6, providing a mechanical gear device in the power transmission mechanism is reliable because it receives torque fluctuations on the tooth surface. It is generally considered to be sexually undesirable. However, in the present invention, since the gear device 8 is connected to the load side of the electromagnetic coupling 18, the output shaft 11 of the prime mover 5
Torque fluctuations in are sufficiently absorbed by the electromagnetic coupling 18 and are not transmitted to the gear device 8. In other words, the electromagnetic coupling 18 not only has a speed reduction mechanism, but also serves as a protection device for the gear device 8. The capacity of this gear device 8 corresponds to that of the rotating electric machine 7, and may be n 1 /n 0 of the capacity of the prime mover 5. For example, when transmitting power from a prime mover output of 10,000 kW,
The rotation speed of the prime mover output shaft 11 is 100 rpm, and the load is 6.
If the rotation speed of is 50 rpm, the capacity of the gear device 8 may be 5,000 KW.

第2図の電磁継手18における一方の回転子2
は界磁巻線20が巻かれた界磁回転子であり、界
磁極23を結合部19で結合する。この界磁極2
3の極表面に設けられた制動巻線21は籠形誘導
機の回転子巻線のように制動巻線相互間を短絡す
る。原動機5の出力軸11にトルク変動が起ると
そのような変動は電磁継手の空隙のため負荷側つ
まり歯車装置8の方へ伝わるのを防ぐのである。
換言すれば伝達するトルク変動の振幅を減衰させ
るのである。
One rotor 2 in the electromagnetic coupling 18 in FIG.
is a field rotor around which a field winding 20 is wound, and the field poles 23 are coupled at a coupling portion 19. This field pole 2
The damper winding 21 provided on the pole surface of the damper 3 short-circuits the damper windings like the rotor winding of a cage induction machine. When torque fluctuations occur on the output shaft 11 of the prime mover 5, such fluctuations are prevented from being transmitted to the load side, that is, the gear device 8, due to the gap in the electromagnetic coupling.
In other words, the amplitude of the transmitted torque fluctuation is attenuated.

以上、本発明を公知特許出願公開昭53−35848
号と比較し、構造上次の基本的相異点がある。す
なわちa固定子を持つ回転電気機械の出力軸と電
磁継手の負荷側回転子の間に小歯車と大歯車のか
み合わせになる歯車装置が結合される。b電磁継
手の界磁極に制動巻線が設けられる。本発明では
このような構造上の特長によつて公知特許出願公
開昭53−35848号とは異なる次のような作用効果
の特長を持つのである。
As mentioned above, the present invention has been disclosed as a publicly known patent application published in 1983-35848.
There are the following basic differences in structure compared to the No. That is, a gear device that meshes with small gears and large gears is coupled between the output shaft of the rotating electrical machine having the a stator and the load-side rotor of the electromagnetic coupling. b A damper winding is provided at the field pole of the electromagnetic joint. Owing to these structural features, the present invention has the following operating and effect features that are different from those of the known patent application published in Japanese Patent Application Publication No. 53-35848.

(1) 歯車装置8を設けることにより前記(6)式で
n0/n2=r×p2/p1+1の値を8にしたい場
合、回転電気機械7の極数p2と電磁継手18の
極数p1をそれぞれ28極と4極にすれば、r=1
となる。これをr=7とすれば、p2もP1も共に
4極になる。r=1は歯車装置8を設けない場
合であり、r=7は歯車装置の減速比である。
この両者を比較し、歯車装置8のない特許出願
公開昭53−35848号の場合、回転電気機械7の
極数が28極に対し、本発明の場合、回転電気機
械7の極数が4極でよいことになる。(1)(2)式に
おいてn1=420rpm、n0=480rpm、n2=60rpm
とし、p1=4とすると、f=4×420/120=14
Hz、そこで(4)式においてp2=4の場合、n3
420rpm、又p2=28の場合、n3=60rpm、従つ
て両者が同一容量で例えば10000KWとすると、
歯車装置8のある場合とない場合の定格はそれ
ぞれ次のようになる。すなわち10000KW、14
Hz、420rpm、4極に対し、10000KW、14Hz、
60rpm、28極である。同一出力、同一周波数の
もとに、一方が420rpm、4極に対し、他方が
60rpm、28極であるから、出しうるトルクを比
較すると、前者は後者のトルクの1/7ですむ。
回転電気機械の寸法と重量を決定するものはそ
の出しうるトルクによると云うのが公知の事で
ある。そこで本発明のように歯車装置8がある
場合では、ない場合にくらべて固定子を持つ回
転電気機械の寸法重量は小形軽量になることが
判る。配列上の点を考えると、特許出願公開昭
53−35848号では電磁継手の回転子から負荷に
到る間に固定子式回転電気機械があり、その寸
法が大形となるから、原動機から電磁継手を経
て固定子を持つ回転電気機械を経て負荷に到る
所謂長さ或いは軸方向の寸法は非常に大きくな
らざるを得ない。本発明ではこのような大形の
回転電気機械の代りに歯車装置8が介在し、そ
れが明らかに上記特許出願公開昭53−35848号
における回転電気機械の寸法にくらべて小形で
あり、動力伝達装置の軸方向の寸法が大きく節
約され、配列上極めて有利な結果になると云う
著しい作用効果の特長が得られる。このことは
船舶の機関室内の配列を考慮する場合などに極
めて重要な作用効果の特長と云える。
(1) By providing the gear device 8, the above formula (6) can be
If you want to set the value of n 0 /n 2 = r×p 2 /p 1 +1 to 8, if you change the number of poles p 2 of the rotating electrical machine 7 and the number of poles p 1 of the electromagnetic coupling 18 to 28 poles and 4 poles, respectively. , r=1
becomes. If this is set to r=7, both p 2 and P 1 become four poles. r=1 is the case where the gear device 8 is not provided, and r=7 is the reduction ratio of the gear device.
Comparing the two, in the case of Patent Application Publication No. 1983-35848 without a gear device 8, the number of poles of the rotating electrical machine 7 is 28 poles, whereas in the case of the present invention, the number of poles of the rotating electrical machine 7 is 4 poles. That's a good thing. In equations (1) and (2), n 1 = 420 rpm, n 0 = 480 rpm, n 2 = 60 rpm
and p 1 = 4, then f = 4 x 420/120 = 14
Hz, so if p 2 = 4 in equation (4), n 3 =
420rpm, and when p 2 = 28, n 3 = 60rpm. Therefore, if both have the same capacity and are, for example, 10000KW,
The ratings with and without the gear device 8 are as follows. i.e. 10000KW, 14
Hz, 420rpm, 4 poles, 10000KW, 14Hz,
60rpm, 28 poles. Under the same output and frequency, one side is 420rpm, 4 poles, and the other side is 420rpm.
Since it has 60 rpm and 28 poles, when comparing the torque that can be produced, the former is only 1/7 of the torque of the latter.
It is well known that the size and weight of a rotating electrical machine is determined by the torque it can produce. Therefore, it can be seen that when the gear device 8 is provided as in the present invention, the dimensions and weight of the rotating electric machine having the stator are smaller and lighter than when the gear device 8 is not provided. Considering the arrangement, the patent application publication date
In No. 53-35848, there is a stator-type rotating electrical machine between the rotor of the electromagnetic coupling and the load, and since its size is large, the rotating electrical machine with the stator is connected from the prime mover through the electromagnetic coupling. The so-called length or axial dimension of the load must be very large. In the present invention, a gear device 8 is interposed in place of such a large-sized rotating electric machine, and it is clearly smaller in size than the rotating electric machine in the above-mentioned patent application publication No. 53-35848, and is capable of transmitting power. The axial dimensions of the device are greatly saved and significant operational advantages are obtained which result in very advantageous arrangement results. This can be said to be an extremely important feature when considering the arrangement in the engine room of a ship.

(2) 電磁継手の界磁極に制動巻線を設ける構造上
の特長によつて本発明では次のような作用効果
の特長が得られる。同期電動機としての電磁継
手の負荷が変化すると、その負荷角δが変化す
る。例えば第3図に示すように、電磁継手の同
期電動機としての定格以下の出力のもとで、負
荷角δ2で運転している時、負荷が次第に増加し
た場合、新らしい負荷角δ4に落ちつく。然し負
荷が角激に増すと、回転子の慣性のために、す
ぐにはδ4に移ることが出来ない。したがつて新
負荷に対して回転電気機械7と電磁継手18の
負荷側回転子1の発生トルクが不足し、それら
電動機の面から見て回転子が減速し、その負荷
角を増すが、それと同時に、発電機としての電
磁継手の発生電力が不足するので、電磁継手1
8の原動機側回転子2はその面からも減速して
発電機としての電磁継手18の負荷角δは次第
に増加する。第3図では横軸に時間tを縦軸に
負荷角δを示す。
(2) Due to the structural feature of providing a damper winding at the field pole of the electromagnetic joint, the present invention provides the following advantages. When the load on the electromagnetic joint as a synchronous motor changes, its load angle δ changes. For example, as shown in Fig. 3, when the electromagnetic coupling is operating at a load angle δ 2 with an output below the rated output as a synchronous motor, and the load gradually increases, the new load angle δ 4 changes. Calm down. However, when the load increases dramatically, it is not possible to immediately shift to δ 4 due to the inertia of the rotor. Therefore, the torque generated by the rotating electrical machine 7 and the load-side rotor 1 of the electromagnetic coupling 18 is insufficient for the new load, and the rotor decelerates from the perspective of the motor, increasing its load angle. At the same time, since the power generated by the electromagnetic coupling as a generator is insufficient, the electromagnetic coupling 1
The motor side rotor 2 of No. 8 is also decelerated from that point of view, and the load angle δ of the electromagnetic coupling 18 as a generator gradually increases. In FIG. 3, the horizontal axis shows time t, and the vertical axis shows load angle δ.

電磁継手18の発電機としての負荷角δと電磁
継手18の両回転子1と2の回転速度差すなわち
(1)式におけるn1=n0−n2との関係はdδ/dt=n10−n1 となる。この場合、n10は両回転子1と2の回転
速度差の同期回転速度であり、n1はその瞬時値で
ある。第3図の曲線Aの上に沿い、δがδ2から変
化して行き、原動機側回転子2の減速により、回
転速度差n1を減少し、δは次第に増加するが、δ4
に達したときはdδ/dtは最大、すなわち回転速度
差n1は最小になつているためδ4に落ちつくことが
できず、さらに慣性のためδは増し続ける。δ4
上になると、電磁継手18の発電機としての発生
出力が負荷出力よりも大になるので、回転子間の
回転速度差n1は大きくなり、原動機側回転子2は
加速され、δ2からδ4に達するまでに回転子2が放
出した運動エネルギーをふたたび吸収して、n1
両回転子1と2の回転速度差の同期回転速度n10
に回復し、dδ/dt=0となつた時、負荷角δ5に達
し、発生出力は負荷出力よりはるかに大きくなつ
ている。このため回転子2は同期速度以上にな
り、ふたたびδ4を通過するときは回転子2の回転
速度は最大となり、dδ/dt=n10−n1は大きく負
の値をとり、最初の負荷角δ2近くまでもどること
になる。このようにしてδはδ4を中心として前後
に周期的な変動を起こし、電気的および機械的損
失のため、振幅が次第に減衰してδ4に落ち着くま
でにしばらく時間がかゝる。結果として回転子2
は加速と減速の振動を繰り返すことになる。然
し、このような最終的な落ち付きを得る場合は良
いが、この変動が助長されて、激しい振動が起こ
る現象があり、これを乱調と云い、乱調が激しく
なると、同期はずれを起こすことがある。第3図
でBなる曲線は安定限界の曲線を示し、その時の
δはδ3であり、この値を越えるCなる曲線の場合
は不安定で、同期はずれとなる。乱調が起これ
ば、界磁巻線を設けた回転子2は電機子電流のつ
くる回転磁界に対して前後に動揺するから、磁極
面にうず電流が流れ、この振動を制動するように
働らくが、この効果をさらに強めるために、磁極
片に制動巻線を設け、本発明のようにするのであ
る。この巻線はδが一定のときには何の作用もし
ないが、δが変動すると、回転磁束を切ることに
よつて電流が流れ、回転磁束との間に制動トルク
を生じ、δを一定に保つように作用するのであ
る。それにより安定度を高めうる。
The load angle δ of the electromagnetic coupling 18 as a generator and the rotational speed difference between the two rotors 1 and 2 of the electromagnetic coupling 18, i.e.
The relationship between n 1 =n 0 −n 2 in equation (1) is dδ/dt=n 10 −n 1 . In this case, n 10 is the synchronous rotational speed of the rotational speed difference between both rotors 1 and 2, and n 1 is its instantaneous value. Along the curve A in FIG. 3, δ changes from δ 2 , and due to the deceleration of the prime mover side rotor 2, the rotational speed difference n 1 decreases, and δ gradually increases, but δ 4
When dδ/dt reaches the maximum, that is, the rotation speed difference n 1 has become the minimum, so it cannot settle down to δ 4 , and δ continues to increase due to inertia. When δ 4 or more, the output generated by the electromagnetic coupling 18 as a generator becomes larger than the load output, so the rotational speed difference n 1 between the rotors increases, the prime mover side rotor 2 is accelerated, and δ 2 The kinetic energy released by rotor 2 is absorbed again until it reaches δ 4 from
When dδ/dt=0, the load angle δ 5 is reached and the generated output is much larger than the load output. Therefore, rotor 2 reaches the synchronous speed or higher, and when it passes through δ 4 again, the rotational speed of rotor 2 reaches its maximum, and dδ/dt=n 10 −n 1 takes a large negative value, and the initial load It will return to near the angle δ 2 . In this way, δ periodically fluctuates back and forth around δ 4 , and it takes some time for the amplitude to gradually attenuate and settle to δ 4 due to electrical and mechanical losses. As a result rotor 2
will repeat oscillations of acceleration and deceleration. However, although it is good when such a final calm is obtained, there is a phenomenon in which this fluctuation is exacerbated and violent vibrations occur. This is called disorder, and if the disorder becomes severe, it may cause a loss of synchronization. . In FIG. 3, the curve B shows the stability limit curve, and δ at that time is δ 3. If the curve C exceeds this value, it is unstable and will be out of synchronization. If disturbance occurs, the rotor 2 equipped with field windings will oscillate back and forth in response to the rotating magnetic field created by the armature current, and eddy currents will flow to the magnetic pole faces and work to dampen this vibration. However, in order to further enhance this effect, a brake winding is provided on the magnetic pole piece, as in the present invention. This winding has no effect when δ is constant, but when δ fluctuates, current flows by cutting off the rotating magnetic flux, creating a braking torque between the rotating magnetic flux and keeping δ constant. It acts on This can improve stability.

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

第1図は本発明の具体的な電気接続図であり、
第2図はその部分接続図である。第3図は本発明
の装置の動作図である。次の図の主要な部分をあ
らわす符号には下記のようなものがある。 1:電磁継手の一方の回転子、2:電磁継手の
他方の回転子、3:スリツプリング、4:スリツ
プリング、5:原動機、6:負荷、7:回転電気
機械、8:歯車装置、9:大歯車、10:ピニオ
ン、11:原動機5の出力軸、12:電磁継手1
8の出力軸、13:整流装置、14:電気接続電
線、15:整流装置の交流側接続電線、16:整
流装置の直流接続電線、17:回転電気機械の出
力軸、18:電磁継手、19:界磁極の結合部、
20:界磁巻線、21:制動巻線、22:電磁継
手の電機子巻線、23:界磁極。
FIG. 1 is a specific electrical connection diagram of the present invention,
FIG. 2 is a partial connection diagram thereof. FIG. 3 is an operational diagram of the apparatus of the present invention. The following symbols represent the main parts of the figure below. 1: One rotor of the electromagnetic coupling, 2: The other rotor of the electromagnetic coupling, 3: Slip ring, 4: Slip ring, 5: Prime mover, 6: Load, 7: Rotating electric machine, 8: Gear device, 9 : Large gear, 10: Pinion, 11: Output shaft of prime mover 5, 12: Electromagnetic coupling 1
8 output shaft, 13: rectifier, 14: electrical connection wire, 15: AC side connection wire of rectifier, 16: DC connection wire of rectifier, 17: output shaft of rotating electrical machine, 18: electromagnetic coupling, 19 : Field pole coupling part,
20: Field winding, 21: Brake winding, 22: Armature winding of electromagnetic joint, 23: Field pole.

Claims (1)

【特許請求の範囲】[Claims] 1 相対的に回転し、相対向する二つの回転子を
有し、少なくともその一方の回転子に電機子巻線
を有する電磁継手の負荷側回転子と大歯車を結合
し、一方固定子を持つ回転電気機械の回転子と結
合した小歯車を上記大歯車とかみ合わせて減速歯
車装置を造ることにより、上記固定子を持つ回転
電気機械の回転子の出力軸から上記減速歯車装置
を経て負荷へ減速動力伝達しうるように配列し、
一方電磁継手の負荷側回転子により直接負荷を駆
動すべく、電磁継手の負荷側回転子と負荷の間を
機械的に結合すると共に、この電磁継手の他方の
回転子を原動機で回転駆動せしめるように配列
し、而も上記固定子を持つ回転電気機械と上記電
磁継手の電機子巻線間を電気接続することによつ
て上記固定子を持つ回転電気機械が電磁継手の電
気出力端子より電力を受けるように配列し、原動
機の出力軸からの出力を電磁継手を経て、一方は
直接に機械力として負荷を駆動し、他方は電磁継
手の電気出力としてこれを固定子を持つ回転電気
機械へ興え、それから変換された機械出力を上記
減速歯車装置を経て負荷へ動力伝達するように配
列し、上記電磁継手の回転子の界磁極の極表面に
制動巻線を設け、籠形誘導機の回転子巻線のよう
に制動巻線相互間を短絡することを特長とする原
動機駆動動力伝達装置。
1. An electromagnetic coupling that has two rotors that rotate relative to each other and that face each other, at least one of the rotors has an armature winding, and the load side rotor and large gear are coupled, and one of the rotors has a stator. A small gear connected to the rotor of the rotating electrical machine is meshed with the large gear to create a reduction gear device, thereby reducing the speed from the output shaft of the rotor of the rotating electrical machine having the stator to the load via the reduction gear device. Arranged to transmit power,
On the other hand, in order to directly drive the load with the load-side rotor of the electromagnetic coupling, the load-side rotor of the electromagnetic coupling and the load are mechanically coupled, and the other rotor of the electromagnetic coupling is rotationally driven by the prime mover. By electrically connecting the rotating electric machine with the stator and the armature winding of the electromagnetic joint, the rotating electric machine with the stator receives power from the electrical output terminal of the electromagnetic joint. The output from the output shaft of the prime mover passes through the electromagnetic coupling, and one directly drives the load as mechanical force, while the other uses the electromagnetic coupling's electrical output to drive a rotating electrical machine with a stator. Then, the converted mechanical output is arranged so as to transmit power to the load via the reduction gear device, and a brake winding is provided on the pole surface of the field pole of the rotor of the electromagnetic joint, and the rotation of the cage induction machine is A prime mover drive power transmission device characterized by short-circuiting braking windings like child windings.
JP5907280A 1980-05-02 1980-05-02 Transmission device for motive power of prime mover Granted JPS56156420A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5907280A JPS56156420A (en) 1980-05-02 1980-05-02 Transmission device for motive power of prime mover

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5907280A JPS56156420A (en) 1980-05-02 1980-05-02 Transmission device for motive power of prime mover

Publications (2)

Publication Number Publication Date
JPS56156420A JPS56156420A (en) 1981-12-03
JPH0221216B2 true JPH0221216B2 (en) 1990-05-14

Family

ID=13102776

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5907280A Granted JPS56156420A (en) 1980-05-02 1980-05-02 Transmission device for motive power of prime mover

Country Status (1)

Country Link
JP (1) JPS56156420A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6173569A (en) * 1984-09-15 1986-04-15 Fukuo Shibata Prime mover drive power transmission
JP5630303B2 (en) * 2011-02-08 2014-11-26 いすゞ自動車株式会社 Non-contact power transmission cutoff device
JP2014053979A (en) * 2012-09-05 2014-03-20 Toshiba Corp Rotating electrical apparatus and wind-power generation system

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5335848A (en) * 1976-09-14 1978-04-03 Kawasaki Heavy Ind Ltd Magnetic gear equipment

Also Published As

Publication number Publication date
JPS56156420A (en) 1981-12-03

Similar Documents

Publication Publication Date Title
JPS62501188A (en) variable speed constant frequency
US4447737A (en) Variable frequency induction generator
JP5291880B2 (en) Ship propulsion system
JPH0622410A (en) Electric hybrid vehicle generator
EP1133045A1 (en) Wound-rotor induction motor and energy conversion facility for variable speed electric machine
JP7830714B2 (en) Hybrid radial axial motor
CN107317457B (en) Permanent magnet coupling speed regulating motor
EP0084717B1 (en) Electrical machine
JPH0221216B2 (en)
JPS6277098A (en) Gas turbine generator
CN107332417A (en) Ship direct current networking electric propulsion system based on asynchronous machine self-excitation
US1723857A (en) Electric power system
JP2524575B2 (en) Braking device for variable speed generator motor in variable speed pumped storage generator
JPS61240900A (en) Windmill generator
JPS6135037B2 (en)
JPH0736718B2 (en) Wind power generator
JPH0121720B2 (en)
SU794702A1 (en) Asynchronized synchronous electric machine
RU2779431C1 (en) Controlled cascade synchronous electric drive
CN111293846B (en) Difference frequency type high-frequency motor
RU55224U1 (en) ASYNCHRONOUS MOTOR FOR REDUCED ELECTRIC DRIVE
SU425292A1 (en) TWO-MOTOR ASYNCHRONOUS ELECTRIC DRIVE
EP0653118A4 (en) ROTARY INDUCTION GENERATOR DRIVEN BY A MOTOR FOR GENERATING ELECTRIC CURRENT.
SU872333A1 (en) A.c. electric transmission of autonomous locomotive
SU855907A1 (en) Electric drive control of floating crane