JPH03289344A - Superconducting motor - Google Patents
Superconducting motorInfo
- Publication number
- JPH03289344A JPH03289344A JP8587590A JP8587590A JPH03289344A JP H03289344 A JPH03289344 A JP H03289344A JP 8587590 A JP8587590 A JP 8587590A JP 8587590 A JP8587590 A JP 8587590A JP H03289344 A JPH03289344 A JP H03289344A
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- superconducting coil
- armature
- liquid helium
- motor according
- 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.)
- Granted
Links
- 239000007788 liquid Substances 0.000 claims abstract description 24
- 239000001307 helium Substances 0.000 claims abstract description 21
- 229910052734 helium Inorganic materials 0.000 claims abstract description 21
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 claims abstract description 21
- 230000005855 radiation Effects 0.000 claims description 11
- 239000000463 material Substances 0.000 claims description 5
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical group [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 claims description 2
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 claims description 2
- 229910052782 aluminium Inorganic materials 0.000 claims description 2
- 229910052802 copper Inorganic materials 0.000 claims description 2
- 239000010949 copper Substances 0.000 claims description 2
- PCHJSUWPFVWCPO-UHFFFAOYSA-N gold Chemical group [Au] PCHJSUWPFVWCPO-UHFFFAOYSA-N 0.000 claims description 2
- 229910052737 gold Inorganic materials 0.000 claims description 2
- 239000010931 gold Substances 0.000 claims description 2
- 239000004020 conductor Substances 0.000 claims 1
- 238000001816 cooling Methods 0.000 claims 1
- 230000004907 flux Effects 0.000 abstract description 5
- 230000005291 magnetic effect Effects 0.000 description 12
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 8
- 229910052757 nitrogen Inorganic materials 0.000 description 4
- 238000007796 conventional method Methods 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- 230000005284 excitation Effects 0.000 description 2
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical group [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 1
- 239000002131 composite material Substances 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 239000003302 ferromagnetic material Substances 0.000 description 1
- 230000008595 infiltration Effects 0.000 description 1
- 238000001764 infiltration Methods 0.000 description 1
- 230000014759 maintenance of location Effects 0.000 description 1
- 239000000779 smoke Substances 0.000 description 1
- 239000002470 thermal conductor Substances 0.000 description 1
Landscapes
- Motor Or Generator Cooling System (AREA)
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】 [発明の1」的] (産業上の利用分野) 本発明は超電導モータに関する。[Detailed description of the invention] [First invention] (Industrial application field) The present invention relates to superconducting motors.
(従来の技術)
従来のディスク型コアレスモークは、界磁として永久磁
石が使用されている。(Prior Art) A conventional disk-type coreless smoke uses a permanent magnet as a field.
(発明が解決しようとする課題)
しかして磁気装架は永久磁石の保持磁束密度に制約され
ているので、1.5テラス程度以上のものを得るのは困
難であった。(Problems to be Solved by the Invention) However, since the magnetic equipment is limited by the retention magnetic flux density of the permanent magnet, it has been difficult to obtain a magnetic equipment with a diameter of about 1.5 terraces or more.
それ故に、本発明は、磁束密度を飛躍的に大きくするこ
とを、その技術的課題とする。Therefore, the technical objective of the present invention is to dramatically increase the magnetic flux density.
(課題を解決するための手段)
上記した技術的課題を解決するために講じた手段は、シ
ャフトに固定された円板状アーマチュア、該アーマチュ
アの一方側に配設され円周方向に等間隔で配置された複
数の超電導コイルを備える第1超電導コイル群、前記ア
ーマチュアの他方側に配設され円周方向に等間隔で配置
された複数の超電導コイルを備える第2超電導コイル群
、前記第1及び第2超電導コイル群を冷却する液体ヘリ
ウム容器、前記円板状アーマチュアとの対向面を除く前
記超電導コイルの全面を覆う輻射シールド体、該輻射シ
ールド体を支持する断熱支持体を介して前記液体ヘリウ
ム容器と連結されたハウジングを兼ねる断熱真空容器を
有する超電導モータを構成したことである。(Means for Solving the Problems) The measures taken to solve the above-mentioned technical problems include a disc-shaped armature fixed to a shaft, disposed on one side of the armature at equal intervals in the circumferential direction. a first superconducting coil group comprising a plurality of superconducting coils arranged; a second superconducting coil group comprising a plurality of superconducting coils disposed on the other side of the armature and arranged at equal intervals in the circumferential direction; A liquid helium container that cools the second superconducting coil group, a radiation shield that covers the entire surface of the superconducting coil except for the surface facing the disc-shaped armature, and a heat insulating support that supports the radiation shield, the liquid helium is A superconducting motor is constructed that has an insulated vacuum container that also serves as a housing connected to the container.
(作用)
上記した手段によれば、界磁として超電導コイルを用い
ているので従来に比べて磁束密度を飛躍的に増加させる
ことが出来る。(Function) According to the above-described means, since a superconducting coil is used as the field, the magnetic flux density can be dramatically increased compared to the conventional method.
(実施例)
以下、本発明に従った超電導モータを実施例に基づき説
明する。(Example) Hereinafter, a superconducting motor according to the present invention will be described based on an example.
第1図において、超電導モータlOはシャフト11を備
える。シャフト11には円板状のアーマチュア12が固
定されており、このアーマチュア12を挟んで1対の超
電導コイル群13が対向している。各超電導コイル群1
3は、円周方向に均等の間隔で配設された複数の超電導
コイル13aは反対側の対応する超電導コイル13aと
同軸となっている。この1対の超電導コイル群13は、
界磁コイルたるヘルムホルツコイルを形成する。In FIG. 1, a superconducting motor IO includes a shaft 11. As shown in FIG. A disc-shaped armature 12 is fixed to the shaft 11, and a pair of superconducting coil groups 13 are opposed to each other with the armature 12 in between. Each superconducting coil group 1
3, a plurality of superconducting coils 13a arranged at equal intervals in the circumferential direction are coaxial with corresponding superconducting coils 13a on the opposite side. This pair of superconducting coil groups 13 are
Forms a Helmholtz coil, which is a field coil.
各超電導コイル群13はトランスファーチューブ19と
連結された環状の液体ヘリウム容器14の中に固定され
ている。この液体ヘリウム容器14は、断熱支持体17
を介して、モータハウジングを兼ねる断熱真空容器16
に固定されている。Each superconducting coil group 13 is fixed in an annular liquid helium container 14 connected to a transfer tube 19 . This liquid helium container 14 has a heat insulating support 17
via an insulated vacuum container 16 that also serves as a motor housing.
is fixed.
トランスファーチューブ19の具体的構造は図示こそさ
れないが、1本の断熱真空配管並びにその中に挿通され
た液体ヘリウム供給管、蒸発ヘリウム排出管、液体窒素
供給管及び液体窒素排出管から構成されている。液体ヘ
リウム容器14と断熱真空容器16との間には熱良導体
(例えばアルミニューム)で形成された輻射シールド体
15が設けられており、この輻射シールド体15が、環
状アーマチュア12との対向面を除く各超電導コイル1
3aの全面を覆っている。Although the specific structure of the transfer tube 19 is not shown, it is composed of a single insulated vacuum pipe, a liquid helium supply pipe, an evaporated helium discharge pipe, a liquid nitrogen supply pipe, and a liquid nitrogen discharge pipe inserted therein. . A radiation shield 15 made of a good thermal conductor (for example, aluminum) is provided between the liquid helium container 14 and the insulating vacuum container 16, and this radiation shield 15 has a surface facing the annular armature 12. Each superconducting coil except 1
It covers the entire surface of 3a.
液体ヘリウム容器14及び真空断熱真空容器16の壁の
内、環状アーマチュア12との対向する部分は薄肉加工
されている。輻射シールド体15の外周には、液体窒素
の通る管が1巻されて且つロー付けされている。また、
断熱支持体17は熱伝導率の低い複合材料で形成されて
おり、輻射シールド体15は断熱支持体17により支持
されている。Of the walls of the liquid helium container 14 and the vacuum insulated vacuum container 16, the portions facing the annular armature 12 are processed to be thin. A tube through which liquid nitrogen passes is wrapped around the outer periphery of the radiation shield body 15 and brazed thereto. Also,
The heat insulating support 17 is made of a composite material with low thermal conductivity, and the radiation shield 15 is supported by the heat insulating support 17.
各超電導コイル13aと円板状アーマチュア12との間
の間隔を短く設定するために、液体ヘリウノ、容器14
及び断熱真空容器16の円板状アーマチュア12との対
向面には、輻射率の低い物質(金・銅等)の鍍金が施さ
れている。また、環状アーマチュア12を挟んで互いに
対向する超電導:1イル13aは強力な磁力で引き合う
ことに鑑み液体ヘリウム容器14と断熱真空容器16と
の間の間隔は太い目に余裕をもって組付ておき、励磁時
に磁力と断熱支持体17の撓みによる力が釣り合う位置
が正しく設定されるようになっている。In order to shorten the distance between each superconducting coil 13a and the disc-shaped armature 12, liquid helium, a container 14
The surface of the heat-insulating vacuum vessel 16 facing the disc-shaped armature 12 is plated with a material having low emissivity (gold, copper, etc.). In addition, in view of the fact that the superconducting coils 13a facing each other with the annular armature 12 in between are attracted to each other by strong magnetic force, the gap between the liquid helium container 14 and the heat-insulating vacuum container 16 is wide enough to allow enough space when assembled. The position where the magnetic force and the force due to the deflection of the heat insulating support body 17 are balanced during excitation is set correctly.
以上の構成における作用を説明する。トランスファーチ
ューブ19を介しての供給により液体ヘリウム容器14
の中に液体ヘリウムが充満されると各超電導コイル13
aは絶対温度で4.2度迄冷却されて超電導状態となる
。このとき、液体ヘリウム容RH4への熱浸入を貼止す
るために液体ヘリウム容器I4は断熱支持体17を介し
て断熱真空容器16に固定されている。しかして断熱支
持体17は液体窒素で冷却された輻射シールド体15を
支持するので、液体ヘリウム容器14への熱浸入の程度
は更に著しく低減される。The operation of the above configuration will be explained. Liquid helium container 14 by supply via transfer tube 19
Each superconducting coil 13 is filled with liquid helium.
A is cooled to an absolute temperature of 4.2 degrees and becomes superconducting. At this time, the liquid helium container I4 is fixed to the heat insulating vacuum container 16 via a heat insulating support 17 in order to prevent heat from entering the liquid helium container RH4. Since the heat insulating support 17 thus supports the radiation shield 15 cooled with liquid nitrogen, the degree of heat infiltration into the liquid helium container 14 is further significantly reduced.
各超電導コイル13aが励磁されると、第2図に矢印で
示されるように、互いに隣接する超電導コイル13a間
に磁力線が発生する。そのため、各超電導コイル13a
の狭い周辺のみに磁界は形成されるので、磁界がモータ
ハウジングの外側には殆ど及ばない。このとき、ブラシ
18を介して円板状アーマチュア12に所定の電流を流
すと、円板状アーマチュア12はローレンツ力により回
転力を得て回転するので、シャツI−11からモータの
出力を取り出すことが出来る。When each superconducting coil 13a is excited, lines of magnetic force are generated between adjacent superconducting coils 13a, as shown by arrows in FIG. Therefore, each superconducting coil 13a
Since the magnetic field is formed only in a narrow periphery of the motor housing, the magnetic field hardly reaches the outside of the motor housing. At this time, when a predetermined current is applied to the disc-shaped armature 12 via the brush 18, the disc-shaped armature 12 obtains rotational force by the Lorentz force and rotates, so that the output of the motor can be extracted from the shirt I-11. I can do it.
以上説明したように、本発明によれば、次のような優れ
た効果を奏する。As explained above, according to the present invention, the following excellent effects are achieved.
(1)界磁として超電導コイルを用いているので従来に
比べて磁束密度を飛躍的に増加させることが出来る。(1) Since a superconducting coil is used as the field magnet, the magnetic flux density can be dramatically increased compared to the conventional method.
(2)磁気回路を閉成するための鉄芯・ヨークその他の
強磁性材を必要としないので、モータ自体の軌量化・小
型化を図ることが出来る。(2) Since no iron core, yoke, or other ferromagnetic material is required to close the magnetic circuit, the motor itself can be made smaller in track and size.
第1図は本発明に係る超電導モータの一実施例の断面図
及び第2図は超電導コイルの励磁状態を説明する図であ
る。
11:シャフト、12
13a :超電導コイル、
15:輻射シールド体、
17:断熱支持体、18
スファーチューブ。
二円板状アーマチュア、
14:液体ヘリウム容器
16:断熱真空容器、
:ブラシ、19ニドランFIG. 1 is a sectional view of an embodiment of a superconducting motor according to the present invention, and FIG. 2 is a diagram illustrating an excitation state of a superconducting coil. 11: Shaft, 12 13a: Superconducting coil, 15: Radiation shield, 17: Heat insulating support, 18 Spher tube. Two disc-shaped armature, 14: Liquid helium container 16: Insulated vacuum container, : Brush, 19 Nidoran
Claims (7)
ーマチュアの一方側に配設され円周方向に等間隔で配置
された複数の超電導コイルを備える第1超電導コイル群
、前記アーマチュアの他方側に配設され円周方向に等間
隔で配置された複数の超電導コイルを備える第2超電導
コイル群、前記第1及び第2超電導コイル群を冷却する
液体ヘリウム容器、前記円板状アーマチュアとの対向面
を除く前記超電導コイルの全面を覆う輻射シールド体、
該輻射シールド体を支持する断熱支持体を介して前記液
体ヘリウム容器と連結されたハウジングを兼ねる断熱真
空容器を有する超電導モータ。(1) A disc-shaped armature fixed to a shaft, a first superconducting coil group including a plurality of superconducting coils disposed on one side of the armature and arranged at equal intervals in the circumferential direction, and a first superconducting coil group provided on the other side of the armature. a second superconducting coil group including a plurality of superconducting coils disposed and arranged at equal intervals in the circumferential direction; a liquid helium container for cooling the first and second superconducting coil groups; and a surface facing the disc-shaped armature. a radiation shield body covering the entire surface of the superconducting coil except for
A superconducting motor having an insulating vacuum container that also serves as a housing and connected to the liquid helium container via an insulating support that supports the radiation shield.
前記断熱真空容器の前記円板状アーマチュアとの対向面
には輻射率の低い材質が鍍金されている超電導モータ。(2) The superconducting motor according to claim 1, wherein surfaces of the liquid helium container and the insulating vacuum container facing the disc-shaped armature are plated with a material having a low emissivity.
である超電導モータ。(3) The superconducting motor according to claim (2), wherein the material with low emissivity is gold.
である超電導モータ。(4) The superconducting motor according to claim (2), wherein the material with low emissivity is copper.
前記断熱真空容器の前記円板状アーマチュアとの対向面
が薄肉加工で形成されている超電導モータ。(5) The superconducting motor according to claim (1), wherein surfaces of the liquid helium container and the insulating vacuum container that face the disc-shaped armature are formed by thin-wall processing.
導体材料で形成されている超電導モータ。(6) The superconducting motor according to claim (1), wherein the radiation shield body is formed of a material with good thermal conductivity.
ニュームである超電導モータ。(7) A superconducting motor according to claim (6), wherein the thermally conductive material is aluminum.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8587590A JP2822570B2 (en) | 1990-03-31 | 1990-03-31 | Superconducting motor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP8587590A JP2822570B2 (en) | 1990-03-31 | 1990-03-31 | Superconducting motor |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH03289344A true JPH03289344A (en) | 1991-12-19 |
JP2822570B2 JP2822570B2 (en) | 1998-11-11 |
Family
ID=13871075
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP8587590A Expired - Fee Related JP2822570B2 (en) | 1990-03-31 | 1990-03-31 | Superconducting motor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2822570B2 (en) |
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0643471A1 (en) * | 1993-09-15 | 1995-03-15 | IMRA MATERIAL R&D CO., LTD. | Superconducting motor |
WO2006068042A1 (en) * | 2004-12-24 | 2006-06-29 | Sumitomo Electric Industries, Ltd. | Axial gap motor |
WO2006068039A1 (en) * | 2004-12-24 | 2006-06-29 | Sumitomo Electric Industries, Ltd. | Axial-gap superconducting motor |
US7315103B2 (en) | 2004-03-03 | 2008-01-01 | General Electric Company | Superconducting rotating machines with stationary field coils |
US7489060B2 (en) | 2006-06-30 | 2009-02-10 | General Electric Company | Superconducting rotating machines with stationary field coils |
US7492073B2 (en) | 2006-06-30 | 2009-02-17 | General Electric Company | Superconducting rotating machines with stationary field coils |
ITMI20112386A1 (en) * | 2011-12-27 | 2013-06-28 | Phase Motion Control S P A | "SYNCHRONOUS GENERATOR MOTOR TO SUPERCONDUCTORS" |
KR20210093941A (en) * | 2018-11-21 | 2021-07-28 | 제네럴 일렉트릭 컴퍼니 | superconducting generator powered by wind turbine |
-
1990
- 1990-03-31 JP JP8587590A patent/JP2822570B2/en not_active Expired - Fee Related
Cited By (18)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5581135A (en) * | 1993-09-15 | 1996-12-03 | Imra Material R & D Co., Ltd. | Superconducting motor |
EP0643471A1 (en) * | 1993-09-15 | 1995-03-15 | IMRA MATERIAL R&D CO., LTD. | Superconducting motor |
US7315103B2 (en) | 2004-03-03 | 2008-01-01 | General Electric Company | Superconducting rotating machines with stationary field coils |
US7821169B2 (en) | 2004-12-24 | 2010-10-26 | Sumitomo Electric Industries, Ltd. | Axial gap type motor |
US7872393B2 (en) | 2004-12-24 | 2011-01-18 | Sumitomo Electric Industries, Ltd. | Axial gap type superconducting motor |
WO2006068039A1 (en) * | 2004-12-24 | 2006-06-29 | Sumitomo Electric Industries, Ltd. | Axial-gap superconducting motor |
JP4690032B2 (en) * | 2004-12-24 | 2011-06-01 | 住友電気工業株式会社 | Axial gap type motor |
JP2006187055A (en) * | 2004-12-24 | 2006-07-13 | Sumitomo Electric Ind Ltd | Axial gap motor |
WO2006068042A1 (en) * | 2004-12-24 | 2006-06-29 | Sumitomo Electric Industries, Ltd. | Axial gap motor |
US7492073B2 (en) | 2006-06-30 | 2009-02-17 | General Electric Company | Superconducting rotating machines with stationary field coils |
US7489060B2 (en) | 2006-06-30 | 2009-02-10 | General Electric Company | Superconducting rotating machines with stationary field coils |
ITMI20112386A1 (en) * | 2011-12-27 | 2013-06-28 | Phase Motion Control S P A | "SYNCHRONOUS GENERATOR MOTOR TO SUPERCONDUCTORS" |
EP2611007A2 (en) | 2011-12-27 | 2013-07-03 | Phase Motion Control S.p.A. | A superconductive synchronous motor generator |
EP2611007A3 (en) * | 2011-12-27 | 2017-04-12 | Phase Motion Control S.p.A. | A superconductive synchronous motor generator |
KR20210093941A (en) * | 2018-11-21 | 2021-07-28 | 제네럴 일렉트릭 컴퍼니 | superconducting generator powered by wind turbine |
CN113316886A (en) * | 2018-11-21 | 2021-08-27 | 通用电气公司 | Superconducting generator driven by wind turbine |
JP2022518327A (en) * | 2018-11-21 | 2022-03-15 | ゼネラル・エレクトリック・カンパニイ | Superconducting generator driven by a wind turbine |
US11764644B2 (en) | 2018-11-21 | 2023-09-19 | General Electric Company | Superconducting generator driven by a wind turbine |
Also Published As
Publication number | Publication date |
---|---|
JP2822570B2 (en) | 1998-11-11 |
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