JP3217531B2 - Superconducting rotor - Google Patents

Superconducting rotor

Info

Publication number
JP3217531B2
JP3217531B2 JP06770193A JP6770193A JP3217531B2 JP 3217531 B2 JP3217531 B2 JP 3217531B2 JP 06770193 A JP06770193 A JP 06770193A JP 6770193 A JP6770193 A JP 6770193A JP 3217531 B2 JP3217531 B2 JP 3217531B2
Authority
JP
Japan
Prior art keywords
superconducting
field winding
rows
slot
connection
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 - Fee Related
Application number
JP06770193A
Other languages
Japanese (ja)
Other versions
JPH06284691A (en
Inventor
正 徳増
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
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP06770193A priority Critical patent/JP3217531B2/en
Publication of JPH06284691A publication Critical patent/JPH06284691A/en
Application granted granted Critical
Publication of JP3217531B2 publication Critical patent/JP3217531B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • 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

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は超電導回転電機における
超電導回転子において、特に巻線取付軸のスロット内に
収納される超電導界磁巻線を構成する超電導導体配置を
改良した超電導回転子に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting rotor in a superconducting rotating electric machine, and more particularly to a superconducting rotor having an improved arrangement of superconducting conductors constituting a superconducting field winding housed in a slot of a winding mounting shaft.

【0002】[0002]

【従来の技術】従来の超電導界磁巻線を備えた超電導回
転子としては、図2に示すような構成のものがある。図
2は超電導回転子の概略的な横断面図である。図2にお
いて、超電導導体からなる界磁巻線1は高強度非磁性鋼
からなる界磁巻線取付軸2のスロット内に納められ、強
固に固定されている。この界磁巻線の内外周部および界
磁巻線部には冷却通路が形成され、これらの冷却通路を
通して界磁巻線取付軸2の内部に有する液体ヘリウム貯
溜部および界磁巻線取付軸2の外周部に配設された液体
ヘリウム容器4内の液体ヘリウム3が循環することによ
り、巻線が冷却されるようになっている。また、液体ヘ
リウム容器4の外周部には、真空断熱層5、輻射熱シー
ルド6および真空容器を構成する常温ダンパ7が同心円
状にそれぞれ配置されている。ところで、このような構
成の超電導回転子において、界磁巻線取付軸2のスロッ
トに収納される界磁巻線としては次のように構成されて
いた。
2. Description of the Related Art As a conventional superconducting rotor having a superconducting field winding, there is one having a configuration as shown in FIG. FIG. 2 is a schematic cross-sectional view of the superconducting rotor. In FIG. 2, a field winding 1 made of a superconducting conductor is housed in a slot of a field winding mounting shaft 2 made of high-strength nonmagnetic steel, and is firmly fixed. Cooling passages are formed in the inner and outer peripheral portions of the field winding and the field winding. Through these cooling passages, the liquid helium reservoir and the field winding attaching shaft inside the field winding attaching shaft 2 are provided. The winding is cooled by circulating the liquid helium 3 in the liquid helium container 4 disposed on the outer peripheral portion of the coil 2. On the outer periphery of the liquid helium container 4, a vacuum heat insulating layer 5, a radiant heat shield 6, and a normal temperature damper 7 constituting the vacuum container are concentrically arranged. By the way, in the superconducting rotor having such a configuration, the field winding housed in the slot of the field winding attachment shaft 2 is configured as follows.

【0003】図3は従来の1スロット分の界磁巻線を示
す図で、この界磁巻線1はスロット内に介挿された下部
絶縁スペーサ8aとサイド絶縁スペーサ8bおよび中間
絶縁スペーサ8cを介挿して超電導導体9を2列にして
納めると共に、スロット底よりこの2列のコイルを同時
に巻上げるダブル・パンケーキ方式で巻回する構成と
し、そのスロット開口側に上部スペーサ8dを挿入して
楔10により固定されている。
FIG. 3 is a view showing a conventional field winding for one slot. This field winding 1 is composed of a lower insulating spacer 8a, a side insulating spacer 8b and an intermediate insulating spacer 8c inserted in the slot. The superconducting conductor 9 is inserted in two rows and inserted, and the two rows of coils are wound simultaneously from the bottom of the slot by a double pancake method. The upper spacer 8d is inserted into the slot opening side. It is fixed by a wedge 10.

【0004】図4はかかる界磁巻線1の1極分の構成を
示した模式図で、界磁コイル間の超電導導体接続部11
が接続側のコイルエンド部に設けられている。ここで、
図4において、1aは界磁巻線直線部、1bは界磁巻線
エンド部である。
FIG. 4 is a schematic diagram showing the configuration of one pole of the field winding 1, and a superconducting conductor connecting portion 11 between the field coils.
Is provided on the coil end portion on the connection side. here,
In FIG. 4, 1a is a field winding linear portion, and 1b is a field winding end portion.

【0005】このような構成の超電導回転子において
は、界磁巻線の最内周のコイルのエンド部内周側での磁
束密度が最も高くなり、クエンチを発生しない安定した
界磁巻線を得るためにはこの高磁束密度部における超電
導導体がクエンチしない最大電流密度を基準として界磁
電流を決めている。しかし、これでは磁束密度の低い部
分の超電導導体の電流密度に過大な裕度を持たせること
になり、超電導導体の能力を有効に利用できず、界磁巻
線の性能が低くなる問題がある。
[0005] In the superconducting rotor having such a configuration, the magnetic flux density on the inner peripheral side of the end portion of the innermost coil of the field winding becomes highest, and a stable field winding without quench is obtained. For this purpose, the field current is determined based on the maximum current density at which the superconducting conductor does not quench in the high magnetic flux density portion. However, this has the problem that the current density of the superconducting conductor in the portion where the magnetic flux density is low has an excessive margin, and the capability of the superconducting conductor cannot be used effectively, and the performance of the field winding is reduced. .

【0006】また、従来の超電導回転子では界磁巻線の
コイル間の接続部をエンド部に設けているため、界磁巻
線の長さが長くなり、超電導回転子全体の寸法が大きく
なる問題がある。
Further, in the conventional superconducting rotor, the connection between the coils of the field winding is provided at the end, so that the length of the field winding becomes longer and the overall size of the superconducting rotor becomes larger. There's a problem.

【0007】さらに、コイル間の接続を行わない側のコ
イルエンド部には接続部を設ける必要がないため、コイ
ルエンド部の長さは長くならないが、この場合には両コ
イルエンド部の長さが異なるために、界磁巻線の磁気中
心位置が不明確になるという問題がある。勿論、接続を
行わないコイルエンド部の長さの接続を行う側と同一と
すれば、磁気中心位置は明確になるが、この場合にはさ
らに界磁巻線長さが長くなって超電導回転子の寸法増大
を招く。
Further, since there is no need to provide a connection portion at the coil end portion on which no connection between the coils is made, the length of the coil end portion does not increase. Therefore, there is a problem that the magnetic center position of the field winding becomes unclear. Of course, if the length of the coil end portion where connection is not made is the same as the connection side, the magnetic center position becomes clear, but in this case the field winding length becomes longer and the superconducting rotor Causes an increase in size.

【0008】このことについては、コイル間の接続をス
ロット内で行う方法があるが、超速応形超電導発電機に
使われる超電導回転子の界磁巻線のように界磁電流を急
変させるような場合には、スロット内の列間および対地
間に大きな電圧が発生するため、スロット内でコイル間
の接続を行うと接続部の絶縁が十分施せないという問題
があった。
[0008] Regarding this, there is a method in which the connection between the coils is made in a slot, but there is a method in which a field current is suddenly changed like a field winding of a superconducting rotor used in a super-speed superconducting generator. In such a case, since a large voltage is generated between the rows and the ground in the slot, there is a problem that if the connection is made between the coils in the slot, the connection cannot be sufficiently insulated.

【0009】[0009]

【発明が解決しようとする課題】このように従来の超電
導回転子においては、界磁巻線の界磁電流密度が高磁束
密度部分における超電導導体がクエンチしない最大電流
密度により制限されるため、超電導導体の性能に比べて
巻線とした場合の性能が低くなる問題がある。また、コ
イルエンド部にコイル間の接続部を設けるため、界磁巻
線が長くなり、超電導回転子の寸法が大きくなる問題が
あった。
As described above, in the conventional superconducting rotor, the field current density of the field winding is limited by the maximum current density at which the superconducting conductor in the high magnetic flux density portion does not quench. There is a problem that the performance when the winding is used is lower than the performance of the conductor. In addition, since the connection between the coils is provided at the coil end, the field winding becomes long, and the size of the superconducting rotor becomes large.

【0010】本発明は上記問題を解決するためになされ
たもので、界磁巻線のエンド部の磁束密度を低減するこ
とによって界磁電流の増加を可能とし、またエンド部の
スロット内でコイル間の接続を行うことにより、寸法が
小さく高性能な界磁巻線を備えた超電導回転子を提供す
ることを目的とする。
SUMMARY OF THE INVENTION The present invention has been made to solve the above-mentioned problem, and it is possible to increase a field current by reducing a magnetic flux density at an end portion of a field winding. It is an object of the present invention to provide a superconducting rotor having a small-sized and high-performance field winding by performing connection between them.

【0011】[0011]

【課題を解決するための手段】本発明は上記の目的を達
成するため、巻線取付軸に設けられたスロットに超電導
界磁巻線を直線部スロット内における超電導導体配置が
2N列にして収納してなる超電導回転子において、エン
ド部スロット内の超電導導体配置を一番内側のスロット
部をN列とし、それより外側のスロット部を2N列と
し、最外周のスロット部をN列にしたものである。ま
た、上記手段に加えてコイル間の接続をコイルエンド部
の超電導導体が2N列巻回されたスロット内で接続する
ようにしたものである。
SUMMARY OF THE INVENTION In order to achieve the above object, the present invention accommodates a superconducting field winding in a slot provided on a winding mounting shaft with superconducting conductors arranged in 2N rows in a straight portion slot. In the superconducting rotor, the innermost slots are arranged in N rows, the outer slots are arranged in 2N rows, and the outermost slots are arranged in N rows. It is. Further, in addition to the above-mentioned means, the connection between the coils is made within a slot where the superconducting conductor of the coil end portion is wound in 2N rows.

【0012】[0012]

【作用】このような構成の超電導回転子とすれば、次の
ような作用効果を得ることができる。一般的に界磁巻線
の磁束分布はコイルエンド部で磁束密度が高くなってお
り、最内周コイルの内周側コイルエンド部で最大とな
る。
With the superconducting rotor having such a configuration, the following operational effects can be obtained. Generally, the magnetic flux distribution of the field winding has a high magnetic flux density at the coil end portion, and becomes maximum at the inner peripheral coil end portion of the innermost peripheral coil.

【0013】本発明ではこの部分のスロット内の列数が
N列と従来のものの半分になるため、この部分での磁束
密度は大幅に低減される。また、磁束密度の高くなるコ
イルエンド部のコーナ部では、全てのコイルがN列ずつ
に分離されるため、この部分での磁束密度も低減され
る。
In the present invention, since the number of rows in the slot at this portion is N rows, which is half of the conventional one, the magnetic flux density at this portion is greatly reduced. Further, in the corner portion of the coil end portion where the magnetic flux density increases, all the coils are separated into N rows, so that the magnetic flux density at this portion is also reduced.

【0014】このように従来の超電導界磁巻線におい
て、磁束密度が高くなる部分の磁束密度が低減されるこ
とによって、界磁巻線電流を従来のものより高め、界磁
巻線の性能を向上させることができる。また、コイル間
の接続をコイルエンド部の超電導導体が2N列からなる
スロット内で行っているため、コイルエンド部に特別な
超電導導体接続のためのスペースが不要となり、しかも
コイルエンド部が短くてすむため、超電導回転子の寸法
を小さく抑えることができる。さらに、両側のコイルエ
ンド部の長さが同一となるため、界磁巻線の磁気中心位
置も明確になる。
As described above, in the conventional superconducting field winding, the magnetic flux density is reduced in the portion where the magnetic flux density is high, so that the field winding current is increased and the performance of the field winding is improved. Can be improved. In addition, since the connection between the coils is made in a slot formed by 2N rows of superconducting conductors at the coil end, no special space for connecting the superconducting conductor is required at the coil end, and the coil end is short. Therefore, the size of the superconducting rotor can be reduced. Further, since the coil end portions on both sides have the same length, the magnetic center position of the field winding becomes clear.

【0015】[0015]

【実施例】以下本発明の一実施例を図面を参照して説明
する。
An embodiment of the present invention will be described below with reference to the drawings.

【0016】図1は本発明による超電導回転子における
超電導界磁巻線の構成例を示すもので、(a)は界磁巻
線の接続を示す模式図であり、(b)は(a)のA−A
線に沿う矢視断面図である。図1に示すように界磁巻線
1は、界磁巻線直線部1aにおいては超電導導体が2列
により構成されているが、界磁巻線エンド部1bでは図
示するように最内周側が1列となり、その外側には直線
部#1コイルの外周側及び#2コイル内周側の2列とな
るスロットが設けられる構成となっている。超電導導体
は直線部のスロット内での2列配置に従ってダブル・パ
ンケーキ方式で巻回され、図1(a)に示すように超電
導導体接続部11でコイル間の接続が行なわれる。
FIG. 1 shows an example of the configuration of a superconducting field winding in a superconducting rotor according to the present invention. FIG. 1 (a) is a schematic view showing the connection of field windings, and FIG. A-A
It is arrow sectional drawing along a line. As shown in FIG. 1, the field winding 1 has two rows of superconducting conductors in the field winding linear portion 1a, but in the field winding end portion 1b, the innermost peripheral side is formed as shown in FIG. One row is provided, and two rows of slots are provided outside the straight section # 1 coil on the outer side and # 2 coil inner side. The superconducting conductor is wound by a double pancake method according to two-row arrangement in the slot of the straight portion, and the connection between the coils is made at the superconducting conductor connecting portion 11 as shown in FIG.

【0017】このように構成することにより、コイルエ
ンド部の磁束密度は最内周側で超電導導体が1列に配置
されるために大幅に低減され、またコイルエンド部のコ
ーナ部では全ての位置で超電導導体が1列配置となるた
め、磁束密度が低減する。
With this configuration, the magnetic flux density at the coil end portion is greatly reduced because the superconducting conductors are arranged in a line at the innermost peripheral side, and all the positions at the corner portions of the coil end portion are reduced. Thus, the superconducting conductors are arranged in one row, so that the magnetic flux density decreases.

【0018】従って、従来の超電導回転子において磁束
密度の高くなるコイルエンド最内周部およびコーナ部で
の磁束密度が低減されるため、従来の構成の界磁巻線よ
り界磁電流を増加させることができる。
Therefore, the magnetic flux density in the innermost peripheral portion and the corner portion of the coil end where the magnetic flux density becomes high in the conventional superconducting rotor is reduced, so that the field current is increased as compared with the field winding of the conventional configuration. be able to.

【0019】また、超電導導体の接続をコイルエンド部
の2列配置の導体内部で行っているため、接続のための
特別のスペースが不要となり、コイルエンド部の長さを
短縮することができる。
Further, since the superconducting conductors are connected inside the conductors arranged in two rows of the coil end portions, no special space for connection is required, and the length of the coil end portions can be shortened.

【0020】この場合、超電導導体を直線部の2列配置
においてダブル・パンケーキ方式で巻回しているので、
コイルエンド部の2列配置のスロットの最上部では列間
の電圧が殆ど発生しないため、図1(b)の断面図に示
すようにコイル間の接続をこの列間中央で行うことによ
り、列間および対地間の絶縁を十分に施すことができ
る。なお、本発明は上記実施例に限定されるものではな
く、その要旨を変更しない範囲で種々変形して実施する
ことができることは勿論である。
In this case, since the superconducting conductor is wound in a double pancake system in a two-row arrangement of straight portions,
Since almost no voltage is generated between the rows at the uppermost portion of the slots arranged in two rows in the coil end portion, the connection between the coils is made at the center between the rows as shown in the cross-sectional view of FIG. The insulation between the ground and the ground can be sufficiently provided. It should be noted that the present invention is not limited to the above-described embodiment, and it goes without saying that various modifications can be made without departing from the scope of the invention.

【0021】[0021]

【発明の効果】以上述べたように本発明にれば、超電導
界磁巻線のコイルエンド部最内周側およびコーナ部の磁
束密度を低減できるので、界磁電流を増大してより強力
な磁場を得ることが可能となり、超電導導体の能力を有
効に利用することができる超電導回転子を得ることがで
きる。また、特別なスペースを設けずにコイル間の接続
が行えるので、界磁巻線の長さが短縮でき、小型の超電
導回転子を得ることができる。
As described above, according to the present invention, the magnetic flux density at the innermost peripheral side of the coil end and the corners of the superconducting field winding can be reduced. A magnetic field can be obtained, and a superconducting rotator capable of effectively utilizing the capability of the superconducting conductor can be obtained. Further, since connection between the coils can be performed without providing a special space, the length of the field winding can be reduced, and a small superconducting rotor can be obtained.

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

【図1】本発明による超電導回転子の一実施例における
超電導界磁巻線の構成を示すもので、(a)は界磁巻線
の接続を示す模式図、(b)は(a)のA−A線に沿う
矢視断面図。
FIGS. 1A and 1B show a configuration of a superconducting field winding in one embodiment of a superconducting rotor according to the present invention, wherein FIG. 1A is a schematic diagram showing connection of the field winding, and FIG. Arrow sectional drawing which follows the AA line.

【図2】従来の2極の超電導回転子の概略的な構成例を
示す横断面図。
FIG. 2 is a cross-sectional view showing a schematic configuration example of a conventional two-pole superconducting rotor.

【図3】従来の1スロット分の界磁巻線を示す図。FIG. 3 is a diagram showing a conventional field winding for one slot.

【図4】従来の界磁巻線の接続構成を示す模式図。FIG. 4 is a schematic diagram showing a connection configuration of a conventional field winding.

【符号の説明】[Explanation of symbols]

1……界磁巻線、2……界磁巻線取付軸、3……液体ヘ
リウム、4……液体ヘリウム容器、5……真空断熱層、
6……輻射熱シールド、7……常温ダンパ、8a,8
b,8c,8d……絶縁スペーサ、9……超電導導体、
10……楔、11……超電導導体接続部。
1 ... field winding, 2 ... field winding mounting shaft, 3 ... liquid helium, 4 ... liquid helium container, 5 ... vacuum insulation layer,
6: radiation heat shield, 7: room temperature damper, 8a, 8
b, 8c, 8d ... insulating spacer, 9 ... superconducting conductor,
10 ... wedge, 11 ... superconducting conductor connection part.

Claims (2)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 巻線取付軸に設けられたスロットに超電
導界磁巻線を直線部スロット内における超電導導体配置
が2N列にして収納してなる超電導回転子において、エ
ンド部スロット内の超電導導体配置を一番内側のスロッ
ト部をN列とし、それより外側のスロット部を2N列と
し、最外周のスロット部をN列にしたことを特徴とする
超電導回転子。
1. A superconducting rotor in which superconducting field windings are accommodated in a slot provided on a winding mounting shaft in a superconducting conductor arrangement in a linear portion slot in 2N rows, and a superconducting conductor in an end portion slot is provided. A superconducting rotator, wherein the innermost slots are arranged in N rows, the outermost slots are arranged in 2N rows, and the outermost slots are arranged in N rows.
【請求項2】 請求項1に記載の超電導回転子におい
て、スロット間の超電導導体の接続をエンド部のスロッ
ト内で行うようにしたことを特徴とする超電導回転子。
2. The superconducting rotator according to claim 1, wherein the connection of the superconducting conductor between the slots is performed within the slot of the end portion.
JP06770193A 1993-03-26 1993-03-26 Superconducting rotor Expired - Fee Related JP3217531B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP06770193A JP3217531B2 (en) 1993-03-26 1993-03-26 Superconducting rotor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP06770193A JP3217531B2 (en) 1993-03-26 1993-03-26 Superconducting rotor

Publications (2)

Publication Number Publication Date
JPH06284691A JPH06284691A (en) 1994-10-07
JP3217531B2 true JP3217531B2 (en) 2001-10-09

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JP06770193A Expired - Fee Related JP3217531B2 (en) 1993-03-26 1993-03-26 Superconducting rotor

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Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CA2201715A1 (en) 1994-10-13 1996-04-25 Anthony J. Rodenbush Variable profile superconducting magnetic coil

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JPH06284691A (en) 1994-10-07

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