JPS6255393B2 - - Google Patents
Info
- Publication number
- JPS6255393B2 JPS6255393B2 JP1240379A JP1240379A JPS6255393B2 JP S6255393 B2 JPS6255393 B2 JP S6255393B2 JP 1240379 A JP1240379 A JP 1240379A JP 1240379 A JP1240379 A JP 1240379A JP S6255393 B2 JPS6255393 B2 JP S6255393B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- rotor
- coil
- magnetic pole
- superconducting coil
- 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
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- Superconductive Dynamoelectric Machines (AREA)
Description
【発明の詳細な説明】
この発明は、超電導発電機の回転子に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a rotor for a superconducting generator.
第1図は、従来の超電導発電機の回転子の断面
を示すものである。第1図において1は回転子、
2は断熱真空容器でダンパを兼ねることもある。
3はコイル取付軸、4は超電導コイルで、以下の
説明では、Nb−Ti(ニオブチタン)から構成さ
れているものとする。5は上記超電導コイル4を
コイル取付軸3に固定するためのウエツジであ
る。6は磁極である。 FIG. 1 shows a cross section of a rotor of a conventional superconducting generator. In Fig. 1, 1 is a rotor;
2 is an insulated vacuum container that may also serve as a damper.
3 is a coil mounting shaft, and 4 is a superconducting coil, which in the following description is assumed to be made of Nb-Ti (niobium titanium). 5 is a wedge for fixing the superconducting coil 4 to the coil mounting shaft 3. 6 is a magnetic pole.
次いで動作について説明する。コイル取付軸3
及び超電導コイル4及びウエツジ5は極低温の液
体ヘリウムないしヘリウムガスで冷却され、Nb
−Tiからなる超電導コイル4は超電導状態に保
たれ、励磁抵抗電力損失なしに通電励磁され、磁
界を発生する。この磁界を発生した回転子1は回
転する事により回転交番磁界を発生し、回転子1
の外側に設けた図示しない電機子コイルに電圧を
発生する。このようにして超電導発電機は構成さ
れている。 Next, the operation will be explained. Coil mounting shaft 3
The superconducting coil 4 and wedge 5 are cooled with cryogenic liquid helium or helium gas, and the Nb
The superconducting coil 4 made of -Ti is maintained in a superconducting state, is energized and excited without loss of excitation resistance power, and generates a magnetic field. The rotor 1 that generated this magnetic field generates a rotating alternating magnetic field by rotating, and the rotor 1
A voltage is generated in an armature coil (not shown) provided on the outside of the motor. The superconducting generator is configured in this way.
従来の回転子1は、以上のようにNb−Tiから
なる超電導コイル4で構成されていた。これは
Nb−Tiは曲げ加工容易で巻線作業をしやすい
が、臨界磁界が低いため、超電導回転子の発生し
うる磁界が比較的低い磁界に制限される。このた
め超電導発電機の磁気装界が2Tesla程度に制限
されるため発電機の寸法重量が一般に期待される
程には小さくならないという深刻な欠点があつ
た。 The conventional rotor 1 was composed of the superconducting coil 4 made of Nb-Ti as described above. this is
Although Nb-Ti is easy to bend and wind, it has a low critical magnetic field, so the magnetic field that can be generated by a superconducting rotor is limited to a relatively low magnetic field. For this reason, the magnetic field of the superconducting generator was limited to about 2 Tesla, so there was a serious drawback that the size and weight of the generator could not be reduced as much as generally expected.
この発明は上記のような従来のものの欠点を除
去するためになされたもので、臨界磁界の高い超
電導線を用いて巻線した超電導コイルを、磁極に
近い部分に適用することにより、磁気装荷の高い
超電導発電機を提供することを目的としている。 This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and by applying a superconducting coil wound using superconducting wire with a high critical magnetic field to the part near the magnetic pole, it is possible to reduce the magnetic loading. The aim is to provide a high-performance superconducting power generator.
以下、この発明の一実施例を図について説明す
る。 An embodiment of the present invention will be described below with reference to the drawings.
第2図において、7は化合物系超電導線材例え
ばNb3Sn(ニオブ3スズ)の巻線を施した第2の
超電導コイルである。本発明の特徴の一つは、上
記化合物超電導線などのように臨界磁界の高い超
電導線による第2の超電導コイル7(以下適宜化
合物超電導コイルと呼ぶ)が、磁極6の近傍に設
けられている事にある。超電導発電機の回転子の
最高磁界は磁極近傍で発生される。従つて、回転
子巻線に通電し得る電流(界磁電流)は、磁極に
最も近い巻線部分の臨界磁界で制限されることに
なる。すなわち磁極から比較的離れている巻線部
分の磁界は十分低く、巻線材料のいかんにかかわ
らず臨界磁界より十分低い値になつている。それ
故、本発明のように磁極近傍に上記した第2の超
電導コイル7を採用することにより、通電し得る
電流を増加させることが可能であり、回転子1の
発生磁界を高くでき、発電機の磁気装荷を高め、
発電機を形、軽量化できる。化合物超電導コイル
7以外のコイルは、安価なNb−Tiの超電導コイ
ル4を使用することにより、回転子1の製造コス
トを低くすることができる。また、化合物超電導
コイル7は磁極6近傍の巾と長さが短かくなり、
他のコイル4に比べ小形ですむ。化合物超電導線
は脆いために曲げ巻線加工が困難であるが、本発
明の磁極近傍におかれた化合物超電導コイル7は
小形であるため巻線加工が容易で、信頼性高く製
作できる事も利点である。 In FIG. 2, numeral 7 denotes a second superconducting coil wound with a compound superconducting wire such as Nb 3 Sn (niobium tritin). One of the features of the present invention is that a second superconducting coil 7 (hereinafter appropriately referred to as a compound superconducting coil) made of a superconducting wire with a high critical magnetic field, such as the compound superconducting wire described above, is provided in the vicinity of the magnetic pole 6. It's true. The highest magnetic field in the rotor of a superconducting generator is generated near the magnetic poles. Therefore, the current (field current) that can be passed through the rotor windings is limited by the critical magnetic field of the winding portion closest to the magnetic poles. That is, the magnetic field in the portion of the winding that is relatively far from the magnetic pole is sufficiently low, and has a value well below the critical magnetic field regardless of the material of the winding. Therefore, by employing the above-mentioned second superconducting coil 7 near the magnetic poles as in the present invention, it is possible to increase the current that can be passed, the magnetic field generated by the rotor 1 can be increased, and the generator increases the magnetic loading of
Generators can be made smaller and lighter. By using the inexpensive Nb-Ti superconducting coil 4 as the coils other than the compound superconducting coil 7, the manufacturing cost of the rotor 1 can be reduced. In addition, the width and length of the compound superconducting coil 7 near the magnetic pole 6 are shortened,
It is smaller than other coils 4. Compound superconducting wires are brittle and difficult to bend and wind, but the compound superconducting coil 7 placed near the magnetic poles of the present invention is small and easy to wind, and the advantage is that it can be manufactured with high reliability. It is.
なお、第2図では化合物超電導コイル7は、磁
極6に近い1対のコイルだけである場合について
示したが、コイル数は単に1対に限るものではな
い。磁極6に近い2対以上のコイルを化合物超電
導コイル7としても本発明の効果が得られる事は
目明であろう。 Although FIG. 2 shows the case where the compound superconducting coil 7 is only one pair of coils close to the magnetic pole 6, the number of coils is not limited to just one pair. It is obvious that the effects of the present invention can be obtained even when two or more pairs of coils close to the magnetic pole 6 are used as the compound superconducting coils 7.
第3図は本発明の他の実施例で、化合物超電導
コイル7の固定されるスロツト8が、磁極方向
(図中矢印A)にほぼ並行に形成されている事が
特徴である。このように構成すると化合物超電導
コイル7は、第4図aに示されるコ字状構造又は
同図bに示すU字状構造などの簡単な構造とな
り、巻線加工や製作が容易になる利点がある。ま
た、化合物超電導コイル7を挿入するスロツトS
は上記のように磁極方向に並行に形成されている
ので第4図に示した化合物超電導コイル7に何ら
機械的な無理(曲げなど)を生ずる事なくスロツ
ト8内にそう入し、固定する事が出来る。 FIG. 3 shows another embodiment of the present invention, which is characterized in that a slot 8 into which a compound superconducting coil 7 is fixed is formed substantially parallel to the magnetic pole direction (arrow A in the figure). With this structure, the compound superconducting coil 7 has a simple structure such as the U-shaped structure shown in FIG. 4a or the U-shaped structure shown in FIG. be. In addition, a slot S into which the compound superconducting coil 7 is inserted is provided.
are formed parallel to the magnetic pole direction as described above, so that the compound superconducting coil 7 shown in FIG. 4 can be inserted into the slot 8 and fixed without causing any mechanical stress (such as bending). I can do it.
第5図は本発明の他の実施例である。化合物超
電導コイル7のそう入される磁極6近傍のスロツ
ト8の軸極6に近い側のスロツト壁面のみが磁極
方向(矢印Aの方向)に平行に形成されており他
の壁面は半径方向に並行に形成されている。この
場合も第6図に示すねじれたU字状又はねじれた
コ字状の形状をなす化合物超電導コイル7を無理
なくスロツト8に挿入できる。9は化合物超電導
コイル7をスロツト8内に挿入後その化合物超電
導コイル7を固定するための絶縁物又は金属から
なる充填物である。この実施例の場合、化合物超
電導コイル7に働く回転遠心力がスロツト8の壁
面に垂直に働くことがないため、スロツト絶縁が
容易になる利点がある。 FIG. 5 shows another embodiment of the invention. Only the slot wall surface on the side near the axial pole 6 of the slot 8 near the magnetic pole 6 into which the compound superconducting coil 7 is inserted is formed parallel to the magnetic pole direction (direction of arrow A), and the other wall surfaces are parallel to the radial direction. is formed. In this case as well, the compound superconducting coil 7 having a twisted U-shape or a twisted U-shape as shown in FIG. 6 can be inserted into the slot 8 without any difficulty. Reference numeral 9 denotes a filler made of an insulator or metal for fixing the compound superconducting coil 7 after it is inserted into the slot 8. In the case of this embodiment, since the rotating centrifugal force acting on the compound superconducting coil 7 does not act perpendicularly to the wall surface of the slot 8, there is an advantage that slot insulation is facilitated.
以上のように、この発明によれば、第2の超電
導コイルを磁極に近い部分に適用するように構成
したので、超電導発電機の磁気装荷が大きくなり
化合物超電導コイルの巻線容易、コイル取付軸へ
の固定容易、さらに化合物超電導コイルの適用が
一部分に限定されるため回転子全体の製作コスト
が低く、かつ信頼性の高いものが得られる効果が
ある。 As described above, according to the present invention, since the second superconducting coil is configured to be applied to a portion close to the magnetic pole, the magnetic loading of the superconducting generator becomes large, the winding of the compound superconducting coil becomes easy, and the coil mounting axis Furthermore, since the application of the compound superconducting coil is limited to only one part, the manufacturing cost of the entire rotor is low, and a highly reliable rotor can be obtained.
第1図は従来の超電導発電機の回転子を示す断
面図、第2図はこの発明の一実施例による超電導
発電機の回転子を示す断面図、第3図、第5図は
それぞれこの発明の他の実施例を示す回転子の断
面図、第4図、第6図はそれぞれ本発明に適用で
きる化合物超電導コイルの例を示す断面斜視図で
ある。
図において、1は回転子、3はコイル取付軸、
4はNb−Ti超電導コイル、6は磁極、7は化合
物超電導コイルである。尚、図中同一符号は同一
或いは相当部分を示す。
FIG. 1 is a sectional view showing a rotor of a conventional superconducting generator, FIG. 2 is a sectional view showing a rotor of a superconducting generator according to an embodiment of the present invention, and FIGS. 3 and 5 are respectively illustrative of the invention. 4 and 6 are cross-sectional perspective views showing examples of compound superconducting coils applicable to the present invention, respectively. In the figure, 1 is the rotor, 3 is the coil mounting shaft,
4 is a Nb-Ti superconducting coil, 6 is a magnetic pole, and 7 is a compound superconducting coil. Note that the same reference numerals in the figures indicate the same or corresponding parts.
Claims (1)
軸の周縁部に固定され、超電導状態で通電励磁さ
れて上記コイル取付軸の径方向に磁極を形成する
複数の超電導コイルとを備えた超電導発電機の回
転子において、上記超電導コイルの内、上記磁極
に近接する超電導コイルを、他の部分の超電導コ
イルを構成する超電導材の臨界磁界より高い臨界
磁界を有する超電導材から構成したことを特徴と
する超電導発電機の回転子。 2 超電導コイルはコイル取付軸に設けられたス
ロツトに挿入されてなることを特徴とする特許請
求の範囲第1項記載の超電導発電機の回転子。 3 磁極に近接する超電導コイルの挿入されるス
ロツトを磁極方向にほぼ並行に設けたことを特徴
とする特許請求の範囲第2項記載の超電導発電機
の回転子。 4 磁極に近接する超電導コイルの挿入されるス
ロツトは、磁極側の壁面を磁極方向に並行にし、
かつ他の壁面を半径方向に並行にしたことを特徴
とする特許請求の範囲第2項記載の超電導発電機
の回転子。 5 磁極に近接する超電導コイルはNb3Sn(ニオ
ブ3スズ)から構成されてなることを特徴とする
特許請求の範囲第1項ないし第4項のいずれかに
記載の超電導発電機の回転子。 6 他の部分の超電導コイルはNb−Ti(ニオブ
チタン)から構成されてなることを特徴とする特
許請求の範囲第5項記載の超電導発電機の回転
子。[Claims] 1. A rotatable coil mounting shaft, and a plurality of superconducting coils fixed to the peripheral edge of the coil mounting shaft and energized in a superconducting state to form magnetic poles in the radial direction of the coil mounting shaft. In the rotor of a superconducting generator, of the superconducting coils, a superconducting coil close to the magnetic pole is made of a superconducting material having a critical magnetic field higher than a critical magnetic field of the superconducting material constituting the other superconducting coils. A rotor for a superconducting generator that is characterized by: 2. A rotor for a superconducting generator according to claim 1, wherein the superconducting coil is inserted into a slot provided in a coil mounting shaft. 3. A rotor for a superconducting generator according to claim 2, wherein slots into which superconducting coils are inserted close to the magnetic poles are provided substantially parallel to the direction of the magnetic poles. 4. The slot in which the superconducting coil is inserted near the magnetic pole should have its wall on the magnetic pole side parallel to the magnetic pole direction.
A rotor for a superconducting generator according to claim 2, wherein the other wall surfaces are parallel to each other in the radial direction. 5. The rotor of a superconducting generator according to any one of claims 1 to 4, wherein the superconducting coil adjacent to the magnetic pole is made of Nb 3 Sn (niobium tritin). 6. The rotor of a superconducting generator according to claim 5, wherein the other portions of the superconducting coil are made of Nb-Ti (niobium titanium).
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1240379A JPS55106077A (en) | 1979-02-05 | 1979-02-05 | Rotor for superconductive generator |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1240379A JPS55106077A (en) | 1979-02-05 | 1979-02-05 | Rotor for superconductive generator |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS55106077A JPS55106077A (en) | 1980-08-14 |
| JPS6255393B2 true JPS6255393B2 (en) | 1987-11-19 |
Family
ID=11804285
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1240379A Granted JPS55106077A (en) | 1979-02-05 | 1979-02-05 | Rotor for superconductive generator |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS55106077A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS57101599A (en) * | 1980-12-11 | 1982-06-24 | Mitsubishi Electric Corp | Exciting system for superconductive generator |
| JPS57101598A (en) * | 1980-12-11 | 1982-06-24 | Mitsubishi Electric Corp | Exciting system for superconductive generator |
| JPS6397488A (en) * | 1986-10-15 | 1988-04-28 | Tech Res & Dev Inst Of Japan Def Agency | Magnetic mine sweeping tool |
-
1979
- 1979-02-05 JP JP1240379A patent/JPS55106077A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS55106077A (en) | 1980-08-14 |
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