JPS6118343A - Rotor of superconductive rotary electric machine - Google Patents

Rotor of superconductive rotary electric machine

Info

Publication number
JPS6118343A
JPS6118343A JP59140795A JP14079584A JPS6118343A JP S6118343 A JPS6118343 A JP S6118343A JP 59140795 A JP59140795 A JP 59140795A JP 14079584 A JP14079584 A JP 14079584A JP S6118343 A JPS6118343 A JP S6118343A
Authority
JP
Japan
Prior art keywords
slot
coil
field coil
superconducting field
superconducting
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.)
Pending
Application number
JP59140795A
Other languages
Japanese (ja)
Inventor
Toshiki Hirao
平尾 俊樹
Koichi Okamoto
岡本 紘一
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP59140795A priority Critical patent/JPS6118343A/en
Publication of JPS6118343A publication Critical patent/JPS6118343A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K55/00Dynamo-electric machines having windings operating at cryogenic temperatures
    • H02K55/02Dynamo-electric machines having windings operating at cryogenic temperatures of the synchronous type
    • H02K55/04Dynamo-electric machines having windings operating at cryogenic temperatures of the synchronous type with rotating field windings
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K3/00Details of windings
    • H02K3/46Fastening of windings on the stator or rotor structure
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Superconductive Dynamoelectric Machines (AREA)

Abstract

PURPOSE:To rigidly hold a superconductive field coil in a simple structure by forming a notch at the top of a tees of a coil mounting shaft, and chamfering the top of the tees integrated with the notch. CONSTITUTION:A superconductive field coil 3 is initially contained at its linear portion 31 and an arc portion 32 in a slot, and then contained at its corner 33 in the slot, thereby containing in the slot. In this case, since no corner is formed at the top 23 of a tees even if a notch 24 is small, the corner 33 of the coil 3 is not affected by the top 23 but readily associated within the slot without labor and time consumption by the chamfered part 27 formed at the top 23 integrated with the notch 24, and the coil can be rigidly held.

Description

【発明の詳細な説明】 〔発明の技術分野〕 この発明は超電導回転電機の回転子、特に超電導回転電
機の回転子、特に超電導界磁コイル取付軸に保持する構
造に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a rotor of a superconducting rotating electrical machine, particularly to a structure for holding the rotor to a superconducting field coil mounting shaft.

〔従来の技術〕[Conventional technology]

従来この種の一般的な回転子として第1図に示すものが
あった。第1図において、(コ)はトルクチューブ、(
2)はトルクチューブ(1)の中央部を形成するコイル
取付軸、(3)はコイル取付軸(2)に固定されている
超電導界磁コイル、(4)はトルクチューブ(1)とコ
イル取付軸(2)を囲繞する常温ダンパ、15)はこの
常温ダンパ(4)とコイル取付軸(2)の間に配設され
ている低温ダンパ、(6)及び(7)はコイル取付軸(
2)のそれぞれ外周部及び側面部に取り付けられたヘリ
ウム外筒及びヘリウム端板、(8)及び(9)はそれぞ
れ駆動側、反駆動側端部軸、00)はこれらの端部軸(
8)。
Conventionally, there has been a rotor shown in FIG. 1 as a general rotor of this type. In Figure 1, (c) is the torque tube, (
2) is the coil mounting shaft that forms the center of the torque tube (1), (3) is the superconducting field coil fixed to the coil mounting shaft (2), and (4) is the torque tube (1) and the coil mounting A room-temperature damper surrounding the shaft (2), 15) is a low-temperature damper disposed between the room-temperature damper (4) and the coil mounting shaft (2), and (6) and (7) are the coil mounting shaft (
The helium outer cylinder and helium end plate are attached to the outer periphery and side surface of 2), respectively, (8) and (9) are the drive side and non-drive side end shafts, 00) are these end shafts (
8).

(9)を軸支する軸受、01)は界磁電流供給用のスリ
ップリング、uりはトルクチューブ(1)に形成或いは
配置されている熱交換器、+131は側部輻射シールド
、(稀は真空部である。
01) is a slip ring for supplying field current, UR is a heat exchanger formed or placed on torque tube (1), +131 is a side radiation shield, (rarely This is the vacuum section.

上記構成からなる超電導回転電機の回転子においては、
コイル取付軸(2)に配設されている超電導界磁コイル
(3)を極低温に冷却するζ、とにより、電気抵抗を零
の状態とし、励磁損失をなくすことにより、この超電導
界磁コイル(3)1ζ強力な磁界を発生させ、固定子(
図示せず)に交流電力を発生させる。この超電導界磁コ
イル(3)を極低温に冷却、保持するために液体ヘリウ
ムを反駆動側端部軸(9)の中央部から導入管(図示せ
ず)を通じ、ヘリウム外筒(6)、ヘリウム端板(7)
により形成される液体ヘリウム容器部に供給する一方、
回転子内部を真空部ホ4)により高真空に床つと共に、
極低温の超電導界磁コイル(3)及びコイル取付軸(2
)(ζ回転トルクを伝えるトルクチューブ(1)を薄肉
円筒とし、且つ熱交換器+12)を設け、このトルクチ
ューブ(1)を通じ極低温部に侵入する熱を極力減らす
構造が最も一般的である。さらに、側面からの輻射によ
り侵入する熱を低減するため、側部軸側シールド+13
1が設けられている。
In the rotor of the superconducting rotating electric machine having the above configuration,
By cooling the superconducting field coil (3) disposed on the coil mounting shaft (2) to an extremely low temperature, the electrical resistance is brought to zero and excitation loss is eliminated. (3) 1ζ Generates a strong magnetic field and stator (
(not shown) to generate AC power. In order to cool and maintain this superconducting field coil (3) at an extremely low temperature, liquid helium is introduced from the center of the non-drive side end shaft (9) through an introduction pipe (not shown) into a helium outer cylinder (6), Helium end plate (7)
While supplying liquid helium to the container formed by
The interior of the rotor is brought to a high vacuum by the vacuum section 4), and
Cryogenic superconducting field coil (3) and coil mounting shaft (2)
) (The most common structure is that the torque tube (1) that transmits the ζ rotational torque is made of a thin-walled cylinder, and a heat exchanger +12 is provided to minimize the heat that enters the cryogenic part through this torque tube (1). . Furthermore, in order to reduce the heat that enters due to radiation from the side, the side shaft side shield +13
1 is provided.

一方、常温ダンパ(4)及び低温ダンパI5)は、固定
子からの高調波磁界をシールドし、超電導界磁コイル(
3)を保護すると共に、電力系統のしよう乱による回転
子振動を減衰させる機能を有する一方、常温ダンパ(4
)は真空外筒としての機能、低温ダンパ15)はヘリウ
ム容器部への軸側シールドとしての機能を兼ねる方式が
一般的である。尚、第1図においては、回転子内部のヘ
リウム導入、排出系を構成する配管類及び回転子に接続
されているヘリウム導入、排出装置は省略している。
On the other hand, the room temperature damper (4) and the low temperature damper I5) shield harmonic magnetic fields from the stator, and the superconducting field coil (
3) and has the function of damping rotor vibrations caused by disturbances in the power system.
) generally functions as a vacuum outer cylinder, and the low-temperature damper 15) also functions as a shaft-side shield for the helium container. In addition, in FIG. 1, piping constituting a helium introduction and discharge system inside the rotor and a helium introduction and discharge device connected to the rotor are omitted.

超電導界磁コイル(3)は第2図fこ示すように直線部
01)、アーク部(3z1 コーナ部(33)を有する
構造となっている。この超電導界磁コイル(3)が運転
中に動くと摩擦熱によって超電導破壊を起こすので、堅
固に保持する必要がある。
The superconducting field coil (3) has a structure having a straight part 01) and an arc part (3z1) and a corner part (33) as shown in Figure 2. If it moves, the superconductor will break due to frictional heat, so it must be held firmly.

又、第1図から判るように、超電導界磁コイル13)は
、ヘリウム外筒(6)、低温ダンパ(5)、常温ダンパ
t41によ−って三重に覆われているので、点検・修理
が非常に困難である。特に、回転電機においては、高い
信頼性が要求されるので、超電導界磁コイル(3)の保
持方法は、超電導回転電機の成否の鍵であるといっても
過言ではない。
Furthermore, as can be seen from Fig. 1, the superconducting field coil 13) is triple-covered by a helium outer cylinder (6), a low-temperature damper (5), and a room-temperature damper T41, so it is difficult to inspect and repair it. is extremely difficult. In particular, since high reliability is required in a rotating electrical machine, it is no exaggeration to say that the method of holding the superconducting field coil (3) is the key to the success or failure of a superconducting rotating electrical machine.

従来この皿の超電導界磁コイル+31の保持方法として
は、特開昭57−166889号公報に記載されるもの
がある。この保持方法は第8図に示すように、超電導界
磁コイル(3)の直線部(31)はコイル取付軸(2)
に形成されたスロットの直線部に収納されたのスロット
に挿入された楔■で保持され、!!3電導界磁コイル(
3)のアーク部□とコーナ部(33)はコイル取付軸(
2)に形成された峻落ち部に収納され保持環(16)と
絶縁つめ物u′?)で保持されている。なお、保持環(
16)の内周側には絶縁カバー@が配設されている。
A conventional method for holding the superconducting field coil +31 of this dish is described in Japanese Patent Laid-Open No. 166889/1989. This holding method is as shown in Figure 8, where the straight part (31) of the superconducting field coil (3) is attached to the coil mounting axis (2).
It is held by a wedge inserted into the slot, which is housed in the straight part of the slot formed in the! ! 3 conductive field coils (
The arc part □ and corner part (33) of 3) are connected to the coil mounting shaft (
2), the retaining ring (16) and the insulating pawl u'? ) is maintained. In addition, the retaining ring (
16), an insulating cover @ is provided on the inner peripheral side.

第4図は第1図のIV−IV線における断面図、即ち、
超電導界磁コイル(3)の直線部(311の円周方向の
断面図を示し、第4図において、(21はコイル取付軸
、13)は超電導界磁コイル、u51は楔、t+81は
コイル取付軸(2)の表面に軸方向に形成されたスロッ
ト、0袋はスロット内絶縁、t20+は楔絶縁である。
FIG. 4 is a sectional view taken along the line IV-IV in FIG. 1, that is,
A circumferential cross-sectional view of the straight part (311) of the superconducting field coil (3) is shown. In Fig. 4, (21 is the coil mounting shaft, 13) is the superconducting field coil, u51 is the wedge, and t+81 is the coil mounting A slot formed in the axial direction on the surface of the shaft (2), 0 bag is insulation in the slot, and t20+ is wedge insulation.

この構成において、超電導界磁コイル13)は、A−A
線を取り巻くように巻回しており、従って、A−A線を
極中心として強力な磁界を発生する。楔(19は超電導
界磁コイル(3)をスロット(旧内に堅固に保持するよ
うに打ち込まれている。従って、コイル保持の信頼性は
高い。
In this configuration, the superconducting field coil 13) is A-A
It is wound around the wire, and therefore generates a strong magnetic field with the A-A wire as the pole center. The wedge (19) is driven to firmly hold the superconducting field coil (3) within the slot. Therefore, the coil holding reliability is high.

又、第5図は超電導界磁コイル(3)のアーク部国の軸
方向の断面図を示し、第5図において、(1)はトルク
チューブ、(2)はコイル取付軸、(3)は超電導界磁
コイル、(6)及び(7)はヘリウム外筒及びヘリウム
端板、(16+は保持環、0ηは絶縁つめ物、し1)は
絶縁敷板、囚は絶縁カバーである。第5図、第8図にお
いて、超電導界磁コイル13)のアーク部国とコーナ部
間はコイル取付軸+21に形成された段落ち部に収納さ
れ、その隙間に絶縁−)め物(1ηが堅固に打ち込まれ
ており、更に、その上から保持環(1ωが焼ばめられて
いる。
Furthermore, Fig. 5 shows an axial cross-sectional view of the arc portion of the superconducting field coil (3). In Fig. 5, (1) is the torque tube, (2) is the coil mounting shaft, and (3) is the Superconducting field coils, (6) and (7) are helium outer cylinders and helium end plates, (16+ is a retaining ring, 0η is an insulating pawl, 1) is an insulating bottom plate, and (1) is an insulating cover. In FIGS. 5 and 8, the area between the arc part and the corner part of the superconducting field coil 13) is housed in a stepped part formed on the coil mounting shaft +21, and an insulating material (1η) is placed in the gap between the arc part and the corner part. It is firmly driven in, and a retaining ring (1ω) is shrink-fitted on top of it.

しかしながら、超N”J+界磁コイル(3)のアーク部
Cl21とコーナ部■、即ち、コイル取付1’Jl (
21に形成された段落ち部における大きな体積を占める
絶縁つめ物Uηの熱収縮量はコイル取付軸(2)や超電
導界磁コイル(3)の熱収縮量に比べ約2程度度大きく
、常温での製作段階で絶縁つめ物Uηを堅固に打ち込ん
でも極低温に冷却すると、絶縁つめ物0りと超電導界磁
コイル(3)との間に隙間が生じる。絶縁つめ物(Iη
は大きな体積を有するのでこの隙間も大きなものとなり
、従って、運転中に振動などの原因で超電導界磁コイル
(3)が動ぎ、摩擦熱によって超電導破壊を起こす恐れ
がある。
However, the arc part Cl21 and the corner part ■ of the super N''J+ field coil (3), that is, the coil installation 1'Jl (
The amount of thermal contraction of the insulating pawl Uη, which occupies a large volume in the stepped part formed in 21, is about 2 degrees larger than that of the coil mounting shaft (2) and the superconducting field coil (3), and is Even if the insulating pads Uη are firmly driven in during the manufacturing stage, when the coil is cooled to an extremely low temperature, a gap will be created between the insulating pads Uη and the superconducting field coil (3). Insulating nails (Iη
Since the coil has a large volume, this gap is also large, and therefore, there is a risk that the superconducting field coil (3) may move due to vibrations or the like during operation, and the superconductor may be destroyed due to frictional heat.

この改善案としては、第6図に示すように、超電導界磁
コイル;3)の直線部(311、アーク部(32)、コ
ーナ部□□□)の全体をスロット18)中に収納し楔0
5)で保持する方法があるが、コイル取付軸(2)の外
周側に形成されたスロット(18)の中へ、予め巻線成
形された超電導界磁コイル(3)を組込むことができず
、超電導界磁コイル13)をコイル取付軸(2)のスロ
ット(18)の中へ直接巻線して成形する必要がある。
As shown in Fig. 6, the proposed improvement is to house the entire straight part (311, arc part (32), corner part □□□) of the superconducting field coil (3) in the slot 18), 0
5), but it is not possible to incorporate the pre-wound superconducting field coil (3) into the slot (18) formed on the outer circumferential side of the coil mounting shaft (2). , it is necessary to form the superconducting field coil 13) by winding it directly into the slot (18) of the coil mounting shaft (2).

しかし、スロット(181中での巻線は作業性が悪く、
巻線に多大の時間と費用が必要となる欠点がある。
However, winding in the slot (181) is difficult to work with.
The disadvantage is that winding requires a lot of time and money.

この改善案としては、第7図〜第12図に示すものがあ
る。第7図はコイル取付軸端部を示す斜視図、第8図は
第7図■−■線における断面図、即ち、コーナ部の断面
図、第9図及び第10図は押え金を示す平面図及び正面
図、第11図は第7図XI−XI線における断面図、第
12図は超電導界コイルの組込み状態を示す斜視図であ
り、第7図〜第12図において、(2)はコイル取付軸
、(3)は超電導界コイル、(31)は直線部、(支)
はアーク部、時はコーナ部、(ISは模、囮はコイル取
付軸(2)に形成されたスロットであり、直線部(18
a)、アーク部(18b)、コーナ部(18C)ニより
構成されている。+19)はスロット内絶縁、+20)
は楔絶縁、C3)はコイル取付軸(2)のティース頂部
、@はスロットf181のコーナ部(1s c)に隣接
するコイル取付軸(2)のティース頂部t23)に形成
された切り欠き部、(至)はこの切り欠き部Q41にポ
ルl−+261により固定され、楔(19を半径方向内
向きに押し付け、超電導界磁コイル(3]のコーナ部(
33jを堅固lこ保持する押え金であり、ボルト5+を
通すボルト穴(25aンが形成されている。
Examples of this improvement plan include those shown in FIGS. 7 to 12. Fig. 7 is a perspective view showing the end of the coil attachment shaft, Fig. 8 is a sectional view taken along the line ■-■ in Fig. 7, that is, a sectional view of the corner portion, and Figs. 9 and 10 are plane views showing the presser foot. FIG. 11 is a sectional view taken along the line XI-XI in FIG. 7, and FIG. 12 is a perspective view showing the assembled state of the superconducting field coil. Coil mounting shaft, (3) is superconducting field coil, (31) is straight part, (support)
is the arc part, time is the corner part, (IS is the model, the decoy is the slot formed in the coil mounting shaft (2), and the straight part (18
It is composed of a), an arc portion (18b), and a corner portion (18C). +19) is insulation in the slot, +20)
C3) is a wedge insulation, C3) is the top of the teeth of the coil mounting shaft (2), @ is a notch formed in the top of the teeth t23) of the coil mounting shaft (2) adjacent to the corner part (1sc) of the slot f181, (to) is fixed to this notch part Q41 by pole l-+261, and the wedge (19) is pressed radially inward, and the corner part of the superconducting field coil (3) (
This is a presser foot that firmly holds the bolt 33j, and has a bolt hole (25a) through which the bolt 5+ is passed.

以上のような構成により、超電導界磁コイル(3)のコ
ーナ部国は押え金(ロ)によってスロットt18+中に
堅固に保持され、超電導界磁コイル13)のアーク部(
32)と直線部01)は楔051によってスロット(1
8)中に堅固に保持される。又、予め巻線成形された超
電導界磁コイル(3)は、第12図に示すように、直線
部C31]とアーク部□□□を初めにスロット(旧中に
収納し、その後コーナ部国をスロットG印中に収納する
ことにより、スロット正中に組込まれる。従って、工作
が容易であり、しかも超電導界磁コイル(3)を堅固に
保持できる。更に、超電導界磁コイル(3)の直線部C
11l、アーク部間、コーナ部(2)の全体をスロット
(淘中に収納し楔05)及び押え金(ロ)で保持する構
造としているので、保持環(161が不要となり、構造
が簡単で点検・修理が容易となると共に経済的効果も高
い。又、予め巻線成形された超電導界磁コイル(3)を
スロットt18+中に組込めるもので、超電導素線を1
ターン毎スロツト形状に合わせてスロット(旧の中へ直
接巻線するような能率の悪い巻線作業に比較し、作業性
が向上した。
With the above configuration, the corner part of the superconducting field coil (3) is firmly held in the slot t18+ by the presser foot (b), and the arc part (
32) and the straight part 01) are connected to the slot (1) by the wedge 051.
8) It is held firmly inside. In addition, as shown in Fig. 12, the pre-wound superconducting field coil (3) is first housed in the slot (the straight part C31) and the arc part □□□, and then the corner part is installed in the slot midline by storing it in the slot G mark. Therefore, the work is easy and the superconducting field coil (3) can be firmly held. Furthermore, the straight line of the superconducting field coil (3) Part C
11l, between the arc parts, and the entire corner part (2) is structured to be held by the slot (wedge 05 that is stored during processing) and the presser foot (b), so the retaining ring (161) is not required and the structure is simple. Inspection and repair are easy, and the economic effect is high.Also, the pre-wound superconducting field coil (3) can be inserted into the slot t18+, and the superconducting wire can be inserted into one
Each turn has a slot that matches the shape of the slot (compared to the old inefficient winding process where the wire was wound directly into the slot, work efficiency has been improved).

しかしながら、この改良案の構造では、超電導界磁コイ
ル(3)をスロット(18)中に組込む際、超電導界磁
コイル(3)のコーナ部(33)をティース頂部t23
1をかわしてスロット118+のコーナ部(i s c
)に収納する作業に問題があった。即ち、第13図に示
すよう(こ、超電導界磁コイル(3)の各ターンは長さ
が異なり、超電導界磁コイル13)の超電導素線(財)
の最内周が最も短くなる。従って、切り欠き部(財)は
、最内周の超電導素線(財)がティース頂部(23)を
越せる大きさにする必要があるところが、超電導回転子
は高速で回転するため、ボルト(イ)には超電導界磁コ
イル(3)と押え金儲の遠心力が作用し、このボルト(
26)の応力は大きなものとなる。この応力を低減する
には、押え金傷)を小さくする。即ち、切り欠き部(財
)を小さくするのが望ましい。このように、機械強度か
ら切り欠き部(241の大きさが制限暴れ、超電導界磁
コイルI31のコーナ部(33)が切り欠き部241に
連なるティース頂部Gの角に当たらないように作業する
ため労力と時間を費やしていた。
However, in the structure of this improved proposal, when the superconducting field coil (3) is assembled into the slot (18), the corner part (33) of the superconducting field coil (3) is
1 and the corner part of slot 118+ (is c
) There was a problem with the storage work. In other words, as shown in FIG.
The innermost circumference of is the shortest. Therefore, the notch needs to be large enough to allow the innermost superconducting wire to pass over the tooth tops (23), but since the superconducting rotor rotates at high speed, the bolts ( ) is acted on by the centrifugal force of the superconducting field coil (3) and the presser foot, and this bolt (
26) The stress becomes large. To reduce this stress, make the presser foot scratches smaller. That is, it is desirable to make the cutout portion (goods) small. In this way, the size of the notch (241) is limited due to mechanical strength, and work must be done to prevent the corner part (33) of the superconducting field coil I31 from hitting the corner of the tooth top G connected to the notch 241. It took effort and time.

〔発明の概要〕[Summary of the invention]

この発明は上記のような従来のものの欠点に鑑がみてな
されたものであり、スロットのコーナ部に隣接するコイ
ル取付軸のティース頂部に切り欠き部を形成し、この切
り欠き部に押え金を締付部材により楔を半径方向内向き
に押し付けるよう固定し、切り欠き部に連なるティース
頂部に面取り部を形成することにより、超電導界磁コイ
ルを堅固に保持することができ、しかも予め巻線成形さ
れた超電導界磁コイルを容易に組込むことができる超電
導回転電機の回転子を提供するものである。
This invention was made in view of the above-mentioned drawbacks of the conventional products, and involves forming a notch at the top of the teeth of the coil mounting shaft adjacent to the corner of the slot, and attaching a presser foot to this notch. By fixing the wedge so as to press it radially inward with the tightening member and by forming a chamfered portion on the top of the teeth that connect to the notch, the superconducting field coil can be firmly held, and it is possible to securely hold the wedge by pre-winding. The present invention provides a rotor for a superconducting rotating electrical machine into which a superconducting field coil can be easily incorporated.

〔発明の一実施例〕[One embodiment of the invention]

以下、この発明の一実施例を第14図、第15図に基づ
いて説明する。第14図は超電導界磁コイルの組込み状
態を示す斜視図、第15図はティース頂部の一部を示す
斜視図であり、第14図、第15図において、(2)は
コイル取付軸、(3)は超電導界磁コイル、01)は直
線部、(32)はアーク部、(33)はコーナ部、■は
コイル取付軸+21に形成されたスロットであり、直線
部(18a)、アーク部(18b)、コーナ部(1s 
c)により構成されている。然)はコイル取付軸(2)
のティース頂部、(至)はスロット(181のコーナ部
(18C)に隣接するコイル取付軸(2)のティース頂
部(23)に形成された切り欠き部、(イ)はこの切り
欠き部241に連なるティース頂部(ハ)に形成された
面取り部である。
An embodiment of the present invention will be described below with reference to FIGS. 14 and 15. Fig. 14 is a perspective view showing the assembled state of the superconducting field coil, and Fig. 15 is a perspective view showing a part of the top of the teeth. 3) is a superconducting field coil, 01) is a straight part, (32) is an arc part, (33) is a corner part, ■ is a slot formed in the coil mounting shaft +21, and the straight part (18a), the arc part (18b), corner part (1s
c). ) is the coil mounting shaft (2)
The top of the tooth (to) is a notch formed in the top of the tooth (23) of the coil mounting shaft (2) adjacent to the corner (18C) of the slot (181), and (A) is the notch formed in this notch 241. This is a chamfered portion formed on the tops (c) of the continuous teeth.

以上のような構成により、超電導界磁コイル(3)は、
直線部(31)とアーク部間を初めにスロット1g+中
に収納し、その後コーナ部(33)をスロット相中に収
納することにより、スロット(]8)中に組込まれる。
With the above configuration, the superconducting field coil (3)
The straight portion (31) and the arc portion are first accommodated in the slot 1g+, and then the corner portion (33) is accommodated in the slot phase, thereby being incorporated into the slot (]8).

その際、切り欠き部(至)に連なるティース頂部圀)に
形成した面取り部(2)によって、切り欠き部(至)が
小さくてもティース頂部(23)の角がないので、超電
導界磁コイル;3)のコーナ部国はティース頂部@に影
響されることなく且つ労力と時間を費やすることなくス
ロット(1B)中lζ容易fこ組込むことができる。
At that time, due to the chamfered part (2) formed on the top part of the tooth (2) connected to the notch part (to), even if the notch part (to) is small, the tooth top part (23) has no corner, so the superconducting field coil ;3) The corner portion can be easily incorporated into the slot (1B) without being affected by the top of the teeth and without expending effort and time.

〔発明の効果〕〔Effect of the invention〕

この発明は以上説明した通り、スロットのコーナ部に隣
接するコイル取付軸のティース頂部に切り欠き部を形成
し、この切り欠き部に押え金を締付部材により楔を半径
方向内向きに押し付けるよう固定し、切り欠き部に連な
るティース頂部fこ面取り部を形成したので、簡単な構
造で超電導界磁コイルを堅固に保持することができ、し
かも予め巻線成形された超電導界磁コイルを労力と時間
を費やすることなく容易に組込むことができる信頼性の
高い超電導回転電機の回転子を得ることができる。
As explained above, this invention forms a notch at the top of the teeth of the coil mounting shaft adjacent to the corner of the slot, and presses the wedge radially inward against this notch using the clamping member of the presser foot. By forming a chamfered part on the top part of the tooth f that is fixed and connected to the notch part, the superconducting field coil can be firmly held with a simple structure, and the superconducting field coil, which has been pre-wound, can be moved without labor. It is possible to obtain a highly reliable rotor for a superconducting rotating electrical machine that can be easily assembled without spending much time.

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

第1図は一般的な超電導回転電機の回転子の全体概念を
示す断面図、第2図は第1図における超電導界磁コイル
の巻線後の状態を示す斜視図、第8図は従来の超電導回
転電機の回転子のコイル取付軸端部を示す斜視図、第4
図は第1図■−IV線における断面図、第5図は従来の
超電澗界磁コイルのアーク部を示す断面図、第6図は従
来の他の超電導回転電機の回転子のコイル取付軸端部を
示す斜視図、第7図は従来の他の超電導回転電機の回転
子のコイル取付軸端部を示す斜視図、第8図は第7図■
−■線における断面図、第9図及び第10図は第7図の
押え金を示す平面図及び正面図、第11図は第7図XI
−XI線における断面図、第12図は従来の超電導界磁
コイルの組込み状態を示す斜視図、第18図は第12図
におけるティース頂部の一部を示す斜視図、第14図は
この発明の一実施例による超電導回転電機の回転子の超
電導界磁コイルの組込み状態を示す斜視図、第15図は
第14図におけるティース頂部の一部を示す斜視図であ
る。 図において、(2jはコイル取付軸、(3)は超電導界
磁コイル、Gllは直線部、■はアーク部、(33)は
コーナ部、(151は楔、[8+はスロット、Qga)
は直線部、(18b)はアーク部、(i s c)はコ
ーナ部、(至)はティース頂部、(至)は切り欠き部、
(ハ)は押え金、■は締付部材、弼は面取り部である。 尚、図中同一符号は同−又は相当部分を示す。
Fig. 1 is a sectional view showing the overall concept of a rotor of a general superconducting rotating electric machine, Fig. 2 is a perspective view showing the state of the superconducting field coil in Fig. 1 after winding, and Fig. 8 is a conventional Perspective view showing the end of the coil attachment shaft of the rotor of the superconducting rotating electric machine, No. 4
The figure is a cross-sectional view taken along the line ■-IV in Figure 1, Figure 5 is a cross-sectional view showing the arc portion of a conventional superconducting field coil, and Figure 6 is a coil installation of the rotor of another conventional superconducting rotating electric machine. FIG. 7 is a perspective view showing the shaft end where the coils of the rotor of another conventional superconducting rotating electric machine are attached, and FIG. 8 is the same as FIG. 7.
9 and 10 are a plan view and a front view showing the presser foot in FIG. 7, and FIG. 11 is a sectional view taken along the line
12 is a perspective view showing the assembled state of a conventional superconducting field coil, FIG. 18 is a perspective view showing a part of the tooth top in FIG. 12, and FIG. FIG. 15 is a perspective view showing a state in which a superconducting field coil is installed in a rotor of a superconducting rotating electrical machine according to an embodiment, and FIG. 15 is a perspective view showing a part of the tooth top in FIG. 14. In the figure, (2j is the coil mounting axis, (3) is the superconducting field coil, Gll is the straight part, ■ is the arc part, (33) is the corner part, (151 is the wedge, [8+ is the slot, Qga)
is a straight part, (18b) is an arc part, (is c) is a corner part, (to) is a tooth top, (to) is a notch part,
(C) is the presser foot, ■ is the tightening member, and the upper part is the chamfered part. Note that the same reference numerals in the figures indicate the same or corresponding parts.

Claims (1)

【特許請求の範囲】[Claims] 軸表面に直線部とアーク部を有するスロットが形成され
たコイル取付軸と、このコイル取付軸のスロット中に収
納される超電導界磁コイルと、上記スロットに挿入され
上記超電導界磁コイルを保持する楔と、上記スロットの
直線部とアーク部とのコーナ部に隣接する上記コイル取
付軸のテイース頂部に形成された切り欠き部と、この切
り欠き部に締付部材により固定され上記楔を半径方向内
向きに押し付け上記スロットのコーナ部の上記超電導界
磁コイルを保持する押え金と、上記切り欠き部に連なる
テイース頂部に形成された面取り部とを備えたことを特
徴とする超電導回転電機の回転子。
A coil mounting shaft in which a slot having a straight line portion and an arc portion is formed on the shaft surface, a superconducting field coil housed in the slot of the coil mounting shaft, and a superconducting field coil inserted into the slot to hold the superconducting field coil. a wedge, a notch formed at the top of the tooth of the coil mounting shaft adjacent to the corner of the straight line part and the arc part of the slot; A rotating superconducting rotating electrical machine characterized by comprising: a presser foot that presses inward and holds the superconducting field coil at a corner portion of the slot; and a chamfered portion formed at the top of the teeth that connects to the notch portion. Child.
JP59140795A 1984-07-05 1984-07-05 Rotor of superconductive rotary electric machine Pending JPS6118343A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59140795A JPS6118343A (en) 1984-07-05 1984-07-05 Rotor of superconductive rotary electric machine

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59140795A JPS6118343A (en) 1984-07-05 1984-07-05 Rotor of superconductive rotary electric machine

Publications (1)

Publication Number Publication Date
JPS6118343A true JPS6118343A (en) 1986-01-27

Family

ID=15276915

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59140795A Pending JPS6118343A (en) 1984-07-05 1984-07-05 Rotor of superconductive rotary electric machine

Country Status (1)

Country Link
JP (1) JPS6118343A (en)

Similar Documents

Publication Publication Date Title
US4462152A (en) Method of mounting coils on the rotor of a superconductive rotary electric machine
US20060293189A1 (en) Machine comprising a rotor and a superconducting rotor winding
JPS6118349A (en) Rotor of superconductive rotary electric machine
US4439701A (en) Rotor of a superconductive rotary electric machine
JPS6118343A (en) Rotor of superconductive rotary electric machine
JP2672892B2 (en) Superconducting rotating electric machine rotor
JPS6118351A (en) Rotor of superconductive rotary electric machine
JPS6118344A (en) Rotor of superconductive rotary electric machine
JPS6118352A (en) Rotor of superconductive rotary electric machine
JPS6118347A (en) Rotor of superconductive rotary electric machine
JPS6118348A (en) Rotor of superconductive rotary electric machine
JP2529382B2 (en) Insertion molding method of superconducting field coil in rotor of superconducting rotating electric machine
JPS6118350A (en) Rotor of superconductive rotary electric machine
JPS6118345A (en) Rotor of superconductive rotary electric machine
GB2099231A (en) Rotor for superconductive rotary electric machine
JPS6118346A (en) Rotor of superconductive rotary electric machine
JPS6118353A (en) Rotor of superconductive rotary electric machine
JPS6118354A (en) Rotor of superconductive rotary electric machine
JPH022076Y2 (en)
JPS6118355A (en) Rotor of superconductive rotary electric machine
JPH02211053A (en) Rotor of superconducting rotary electric machine and manufacture thereof
JP2667063B2 (en) Superconducting rotating electric machine rotor
JPH0456548B2 (en)
JPS603555Y2 (en) superconducting coil
JPS63228959A (en) Rotor for superconducting rotary electric machine