JPH01255451A - coreless motor - Google Patents

coreless motor

Info

Publication number
JPH01255451A
JPH01255451A JP63081397A JP8139788A JPH01255451A JP H01255451 A JPH01255451 A JP H01255451A JP 63081397 A JP63081397 A JP 63081397A JP 8139788 A JP8139788 A JP 8139788A JP H01255451 A JPH01255451 A JP H01255451A
Authority
JP
Japan
Prior art keywords
thin film
conducting wire
magnetic flux
rotor
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.)
Granted
Application number
JP63081397A
Other languages
Japanese (ja)
Other versions
JP2746596B2 (en
Inventor
Takeshi Sawada
武 澤田
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP63081397A priority Critical patent/JP2746596B2/en
Priority to US07/220,162 priority patent/US5099162A/en
Publication of JPH01255451A publication Critical patent/JPH01255451A/en
Priority to US08/138,389 priority patent/US5389908A/en
Application granted granted Critical
Publication of JP2746596B2 publication Critical patent/JP2746596B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • Y—GENERAL 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
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Windings For Motors And Generators (AREA)
  • Superconductive Dynamoelectric Machines (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は磁束経路中の巻線に超伝導材を用いたコアレス
モータおよび巻線に用いられる導線に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a coreless motor using a superconducting material for the winding in a magnetic flux path and a conducting wire used for the winding.

[従来の技術] この種のモータのうち、回転子の巻線と鉄心が分離され
たコアレスモータは、鉄心(コア)を有してコイルを構
成するモータに比較し、ヒステリシスロスが無く、また
ヒステリシスロスは交番磁界の周波数に比例することか
ら、特に高速回転によるデイメリットが発生しないこと
、リアクタンス電圧が小さいため整流子での接触によっ
て発生する火花が少なく整流子の損傷が小さいこと、さ
らに回転子の慣性モーメントが小さく、サーボモータに
適していること等の利点を有している。また、巻線の構
成を斜め巻きなど適切に構成すれば、回転におけるコギ
ングを防止することもできる。
[Prior Art] Among these types of motors, coreless motors in which the rotor windings and the iron core are separated have no hysteresis loss and Hysteresis loss is proportional to the frequency of the alternating magnetic field, so there are no disadvantages caused by high-speed rotation, and because the reactance voltage is small, there are fewer sparks caused by contact with the commutator, and damage to the commutator is small. It has the advantage of having a small moment of inertia and being suitable for use with servo motors. Further, if the winding is appropriately configured such as diagonally wound, cogging during rotation can be prevented.

第7図(A)および(B)はそれぞれコアレスモータに
おける回転子の一例を示す斜視図および上記回転子を配
設したコアレスモータの断面図である。
FIGS. 7(A) and 7(B) are a perspective view showing an example of a rotor in a coreless motor, and a sectional view of a coreless motor in which the rotor is provided, respectively.

これら図において、回転子8は、電機子巻線としての導
線2を斜め巻きしたものを円筒形状にし、エポキシ系の
樹脂で固めることによって形成される。回転子8は、回
転軸1と回転子8の底に配設された樹脂等の支持板8^
によって連結されることにより回転子8の回転が回転軸
1に伝達される。
In these figures, the rotor 8 is formed by diagonally winding a conducting wire 2 as an armature winding into a cylindrical shape and hardening it with an epoxy resin. The rotor 8 consists of the rotating shaft 1 and a support plate 8 ^ made of resin or the like disposed on the bottom of the rotor 8.
The rotation of the rotor 8 is transmitted to the rotating shaft 1 by being connected by.

回転@1は、コアレスモータの外側コア5等の構造部材
に設けられた軸受IAおよび1Bによって軸支される。
The rotation @1 is supported by bearings IA and 1B provided in a structural member such as the outer core 5 of the coreless motor.

この構成において、上記構造部材に接続する固定子界磁
としての永久磁石4が、回転子8の内側に配設される。
In this configuration, a permanent magnet 4 serving as a stator field connected to the structural member is disposed inside the rotor 8.

また、回転軸1の一端には整流子3^が取付けられ、ブ
ラシ3Bとの接触によって導線2に流れる電流の方向が
定められる。
Further, a commutator 3^ is attached to one end of the rotating shaft 1, and the direction of the current flowing through the conducting wire 2 is determined by contact with the brush 3B.

第8図は第7図に示した構成の上断面図である。図から
明らかなように、永久磁石4のN極から出た磁束は導線
2を貫いて軟磁性材で形成される外側コア5を通り、再
び導線2を貫いて永久磁石4のS極に至る。このとき、
導線に流れる電流方向6を、磁束の方向に応じて適切に
制御すれば、例えば図中符号7で示す方向に回転子8が
回転する。
FIG. 8 is a top sectional view of the structure shown in FIG. 7. As is clear from the figure, the magnetic flux emitted from the N pole of the permanent magnet 4 passes through the conductor 2, passes through the outer core 5 made of soft magnetic material, and passes through the conductor 2 again to reach the S pole of the permanent magnet 4. . At this time,
If the direction 6 of the current flowing through the conducting wire is appropriately controlled according to the direction of the magnetic flux, the rotor 8 rotates in the direction indicated by the reference numeral 7 in the figure, for example.

ところで、この種のモータ効率は、固定子や回転子の形
状、永久磁石から発生する磁束の量、あるいは導線の電
気抵抗等に依存するものであり、特に導線素材の固有電
気抵抗の低減化は大きな課題であった。
By the way, the efficiency of this type of motor depends on the shape of the stator and rotor, the amount of magnetic flux generated from the permanent magnets, the electrical resistance of the conducting wire, etc., and it is especially important to reduce the specific electrical resistance of the conducting wire material. It was a big challenge.

これに対して、最近の超伝導材開発の進展に伴い、液体
窒素温度で超伝導状態が実現される材料が可能となって
きており、これにより巻線に超伝導材料を用いたコアレ
スモータも提供されるようになってきた。
On the other hand, with the recent progress in the development of superconducting materials, it has become possible to create materials that achieve a superconducting state at liquid nitrogen temperatures, and this has led to the creation of coreless motors that use superconducting materials for the windings. It's starting to be offered.

[発明が解決しようとする課題] しかしながら、超伝導材の導線を用いたコアレスモータ
は、第9図に示すように導線9の断面形状およびその配
列によって、超伝導材を用いたことによる効果が相殺さ
れがちになる。
[Problems to be Solved by the Invention] However, in a coreless motor using conductive wires made of superconducting material, the effect of using superconducting material cannot be achieved due to the cross-sectional shape of the conductive wire 9 and its arrangement, as shown in FIG. They tend to be canceled out.

すなわち、導線9におけるマイスナー効果によって磁力
線は導線9を貫通することができず、図に示すような磁
力線分布14が形成される。これにより、導線9を迂回
するために磁路長が長くなり、かつ磁束通路が狭くなる
ために磁束鎖交面積が小さくなってリラクタンスが増大
し、磁束量が減少する。この結果、導線の電気抵抗がO
になる超伝導材を用いたことによる効率の向上が相殺さ
れてしまうことになる。
That is, due to the Meissner effect in the conducting wire 9, the magnetic lines of force cannot penetrate through the conducting wire 9, and a magnetic force line distribution 14 as shown in the figure is formed. As a result, the magnetic path length becomes longer to bypass the conducting wire 9, and the magnetic flux path becomes narrower, so that the magnetic flux linkage area becomes smaller, the reluctance increases, and the amount of magnetic flux decreases. As a result, the electrical resistance of the conductor is O
The improvement in efficiency achieved by using superconducting materials will be canceled out.

本発明は、上述した観点に鑑みてなされたものであり、
その目的とするところは巻線としての導線に超伝導材を
用いたことによる本来の効果を発揮し得るような効率の
良い形状の超伝導導線を提供し、かつ上記導線を用いた
コアレスモータ等の電気機器を提供することにある。
The present invention has been made in view of the above-mentioned viewpoints,
The purpose is to provide a superconducting wire with an efficient shape that can demonstrate the original effect of using superconducting material for the conductor wire as a winding wire, and to develop coreless motors etc. using the above conductor wire. Our goal is to provide the following electrical equipment.

[課題を解決するための手段] そのために本発明では、導線が、少なくとも1つの平面
を有する金属基板と、金属基板か有する少なくとも1つ
の平面上に形成された超伝導材薄膜とによって構成され
ることを特徴とする。
[Means for Solving the Problems] To this end, in the present invention, a conducting wire is constituted by a metal substrate having at least one flat surface and a superconducting thin film formed on the at least one flat surface of the metal substrate. It is characterized by

また固定子としての磁束発生手段を有し、回転子におけ
る電流路が上述した導線によって構成され、超伝導材薄
膜の膜面が電流路を鎖交する磁束の方向と平行であるこ
とを特徴とする。
It also has a magnetic flux generating means as a stator, the current path in the rotor is constituted by the above-mentioned conducting wire, and the film surface of the superconducting thin film is parallel to the direction of the magnetic flux interlinking the current path. do.

[作 用] 以上の構成によれば、導線によって構成される電流路を
通過する磁束は、マイスナー効果によって受ける影響が
少なく、磁路長が長くなることおよび磁束鎖交の面積が
狭くなることが防止される。
[Function] According to the above configuration, the magnetic flux passing through the current path formed by the conducting wire is less affected by the Meissner effect, and the magnetic path length is increased and the area of magnetic flux linkage is reduced. Prevented.

さらに、常伝導状態においてもモータの回転が可能でか
つ超伝導状態が部分的に破れても抵抗増大による急激な
熱発生等が防止される。
Furthermore, the motor can rotate even in the normal conduction state, and even if the superconductivity state is partially broken, sudden heat generation due to increased resistance is prevented.

[実施例] 以下、図面を参照して本発明の実施例を詳細に説明する
。
[Example] Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

第1図は本発明の一実施例を示す回転子の上断面の一部
を示す図である。第9図に示したのと同様の要素には同
一の符号を付してその説明は省略する。また、第2図(
A)および(B)は第1図に示した回転子のそれぞれ外
観斜視図および展開図である。
FIG. 1 is a diagram showing a part of an upper cross section of a rotor showing an embodiment of the present invention. Elements similar to those shown in FIG. 9 are designated by the same reference numerals, and their explanations will be omitted. Also, Figure 2 (
A) and (B) are an external perspective view and a developed view, respectively, of the rotor shown in FIG. 1.

これら図において、9は巻線としての導線であり、導線
9は、Cu、AI等の良導体で形成される金属基板I3
と、金属基板13の片面に[1i−La−5r−Cu−
0゜Y−Ba−Cu−0,La−[1a−Cu−0等、
希土類金属や遷し金属を含んだセラミックまたは超伝導
金属合金などを一層または複数層堆積した超伝導薄膜l
Oとによって形成される。超伝導薄膜10は抵抗加熱蒸
着またはエレクトロンビーム蒸着、スパッタリング。
In these figures, 9 is a conducting wire as a winding wire, and the conducting wire 9 is a metal substrate I3 formed of a good conductor such as Cu or AI.
and [1i-La-5r-Cu-
0゜Y-Ba-Cu-0, La-[1a-Cu-0, etc.
A superconducting thin film made by depositing one or more layers of ceramic or superconducting metal alloy containing rare earth metals or transitional metals.
It is formed by O. The superconducting thin film 10 is formed by resistance heating evaporation, electron beam evaporation, or sputtering.

メツキ、 CVO等によって形成され、また金属基板1
3の薄膜lOを堆積しない部位はマスクやサセプタによ
って覆われ薄膜lOの堆積が防止される。
The metal substrate 1 is formed by plating, CVO, etc.
The portions of No. 3 where the thin film 1O is not deposited are covered with a mask or a susceptor to prevent the thin film 1O from being deposited.

上述のように形成された導線9によって、第2図(B)
に示すように展開された状態で巻線パターンが定められ
、各導線間は、絶縁接着材11Aが充填されることによ
り巻線パターンが固定される。
By the conductive wire 9 formed as described above, as shown in FIG. 2(B)
A winding pattern is defined in the unfolded state as shown in FIG. 2, and the winding pattern is fixed by filling the space between each conducting wire with an insulating adhesive 11A.

さらに巻線パターンの両面は樹脂11Bによって被覆さ
れる。このように形成した巻線パターンにより円筒形の
回転子8が成形される。
Furthermore, both sides of the winding pattern are coated with resin 11B. A cylindrical rotor 8 is formed by the winding pattern thus formed.

この構成において、第1図に示すように回転子8を通過
する磁束の方向と、超伝導薄膜lOの面がほぼ平行とな
るよう導線9が配設されるため、第9図に示したように
超伝導薄膜lOにおけるマイスナー効果によって磁束経
路が歪められることはほとんど無くなり、リラクタンス
の増大が防止される。この結果、コアレスモータの巻線
に超伝導材を用い、巻線の電気抵抗がOになることが、
そのまま効率向上に結び付くことになる。
In this configuration, as shown in FIG. 1, the conducting wires 9 are arranged so that the direction of the magnetic flux passing through the rotor 8 is almost parallel to the surface of the superconducting thin film IO, so that the conductive wires 9 are arranged as shown in FIG. In this case, the magnetic flux path is hardly distorted by the Meissner effect in the superconducting thin film 10, and an increase in reluctance is prevented. As a result, it is possible to use a superconducting material in the windings of a coreless motor, and the electrical resistance of the windings becomes O.
This will directly lead to improved efficiency.

また、基板13にCu、Ai等の金属を用いることによ
り、超伝導薄膜lOが常伝導状態にあっても導線9には
電流を流すことができ、モータは回転することが可能と
なる。これは、例えば本実施例のモータを超伝導状態が
実現される低温下において使用する場合、その温度にな
るまでモータを回転しながら冷却することができ、モー
タの凍結が防止される。
Further, by using a metal such as Cu or Al for the substrate 13, even if the superconducting thin film IO is in a normal conduction state, current can be passed through the conducting wire 9, and the motor can rotate. For example, when the motor of this embodiment is used at a low temperature where a superconducting state is achieved, the motor can be cooled while rotating until it reaches that temperature, thereby preventing the motor from freezing.

さらに、金属基板の効果は、超伝導が部分的に破れた場
合でも電流が基板13をバイパスとして流れ急激な抵抗
増大によって生ずる熱によるモータへの悪影響を防止で
きる。
Furthermore, the effect of the metal substrate is that even if superconductivity is partially broken, the current flows by bypassing the substrate 13 and can prevent the adverse effect on the motor due to heat caused by a sudden increase in resistance.

さらに加えて、第1図に示すように導線9のピッチをβ
とし、超伝導薄膜10の厚さをtとするとき、tは可能
なかぎり薄いほうがよいが、最大必要電流等を勘案して
、所定の厚さが必要となる。
In addition, the pitch of the conducting wire 9 is β as shown in FIG.
When the thickness of the superconducting thin film 10 is t, it is better that t be as thin as possible, but a predetermined thickness is required in consideration of the maximum required current, etc.

このとき、経験上1〉2tの関係が成立していることが
望ましい。
At this time, it is desirable from experience that the relationship 1>2t holds true.

第3図は巻線パターンの他の実施例を示す。同図に示す
パターンは第2図(B)のパターンと異なり、複数本の
導線9によって巻線パターンを構成している。この場合
、導線9がクロスしている部分が無く回転子厚みを薄く
でとる利点がある。なお、第2図や第3図における巻線
の本数や巻き回数は概念的に示されるものであり、図に
示されるものに限られない。
FIG. 3 shows another embodiment of the winding pattern. The pattern shown in the figure differs from the pattern in FIG. 2(B) in that a plurality of conductive wires 9 constitute a winding pattern. In this case, there is no part where the conducting wires 9 cross, and there is an advantage that the rotor can be made thinner. Note that the number of windings and the number of windings in FIGS. 2 and 3 are shown conceptually, and are not limited to what is shown in the figures.

第4図は導線の他の実施例を示す第1図と同様の1断面
図である。第1図に示す導線の構造と異なるのは、超伝
導薄膜10が金属基板13によって挟まれていることで
ある。この導線9の構造は例えば圧延によるクラッドと
して実現される。
FIG. 4 is a cross-sectional view similar to FIG. 1 showing another embodiment of the conducting wire. What differs from the structure of the conducting wire shown in FIG. 1 is that a superconducting thin film 10 is sandwiched between metal substrates 13. The structure of the conducting wire 9 is realized, for example, as a rolled cladding.

導線9の上述した構成により、超伝導薄膜IOの経時変
化が基板13によって被覆されることにより防止され、
導線9の信頼性が向上する。
With the above-described configuration of the conductive wire 9, deterioration of the superconducting thin film IO over time is prevented by being covered by the substrate 13,
The reliability of the conducting wire 9 is improved.

また、上述した構成の場合、圧延等の加工工程で、超伝
導薄膜を破壊することなく製造することができ、加工上
の利点が大きい。
Moreover, in the case of the above-mentioned structure, the superconducting thin film can be manufactured without being destroyed in a processing step such as rolling, which has a great advantage in processing.

第5図および第6図は導線の他の実施例を示す横断面図
である。
5 and 6 are cross-sectional views showing other embodiments of the conducting wire.

第5図は金属基板13の両側面に超伝導薄膜lOを堆積
した構成を示し、例えばCVDによって薄膜lOが形成
される。
FIG. 5 shows a configuration in which a superconducting thin film 10 is deposited on both sides of a metal substrate 13, and the thin film 10 is formed by, for example, CVD.

第6図は第5図に示した導線において、Cuメツキ13
八によって超伝導薄膜10を保護した構成を示す。
Figure 6 shows Cu plating 13 in the conductor shown in Figure 5.
8 shows a configuration in which the superconducting thin film 10 is protected.

第5図や第6図に示すように薄11%10を2面に配す
ることによって電流の量や薄膜lOの厚さを多様に設定
することが可能となる。
As shown in FIGS. 5 and 6, by arranging the thin 11% 10 on two sides, it becomes possible to variously set the amount of current and the thickness of the thin film 1O.

なお、上述した各実施例ではコアレスモータに関して説
明したが、電流路が固定子、磁束発生源が回転子となっ
ているモータについても本発明はj内用され得る。
Although the above-mentioned embodiments have been described with reference to a coreless motor, the present invention can also be applied to a motor in which the current path is a stator and the magnetic flux generation source is a rotor.

また、上述の各実施例に示した導線は、その超伝導薄膜
の面を磁束経路と平行に配設すれば、例えば変圧器、電
力貯蔵用インダクタ、コイル等の電気機器の性能を向上
させることができる。
In addition, the conducting wires shown in the above-mentioned embodiments can improve the performance of electrical equipment such as transformers, power storage inductors, and coils by arranging the superconducting thin film surface parallel to the magnetic flux path. I can do it.

[発明の効果] 以上の説明から明らかなように本発明によれば導線によ
って構成される電流路を通過する磁束は、マイスナー効
果によって受ける影習が少なく、磁路長°が長くなるこ
とおよび磁束鎖交の面積が狭くなることが防止される。
[Effects of the Invention] As is clear from the above description, according to the present invention, the magnetic flux passing through the current path formed by the conducting wire is less affected by the Meissner effect, and the magnetic path length is increased and the magnetic flux is This prevents the area of linkage from becoming narrower.

さらに、常伝導状態においてもモータの回転が可能でか
つ超伝導状態が部分的に破れても抵抗増大による急激な
熱発生等が防止される。
Furthermore, the motor can rotate even in the normal conduction state, and even if the superconductivity state is partially broken, sudden heat generation due to increased resistance is prevented.

この結果、マイスナー効果によるリラクタンスの増大と
いった、超伝導材を用いたことによる効率の低下が防止
でき、超伝導材の電気抵抗がOになる本来の利点を十分
に発揮したコアレスモータを得ることができた。
As a result, it is possible to prevent a decrease in efficiency due to the use of superconducting materials, such as an increase in reluctance due to the Meissner effect, and to obtain a coreless motor that fully utilizes the inherent advantages of superconducting materials with an electrical resistance of 0. did it.

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

第1図は本発明の一実施例を示すコアレスモータの1断
面図、 第2図(^)および(B)は第1図に示したコアレスモ
ータにおける回転子のそれぞれ斜視図および展開図、 第3図は回転子における巻線パターンの変形例を示す展
開図、 第4図は本発明の他の実施例を示す回転子の1断面図、 第5図および第6図は本発明の他の実施例を示す導線の
横断面図、 第7図(A)はコアレスモータにおける回転子の斜視図
、 第7図(B)は第7図(^)に示した回転子を適用した
コアレスモータの断面図、 第8図および第9図は従来例を示すコアレスモータの1
断面図である。 l・・・回転軸、 2.9・・・導線、 3八・・・整流子、 3B・・・ブラシ、 4・・・永久磁石、 5・・・外側コア、 6・・・電流方向、 7・・・回転方向、 8・・・回転子、 1−0・・・超伝導薄膜、 11A・・・絶縁接着材、 11B・・・樹脂、 13・・・金属基板、 14・・・磁力線分布。 第2 図(A) 第2 図(B) 3A 第31 、、ニー35 図      第6図 6電;尤プ句 第8図 9 々イ云j岬二i−木粗 第9図
FIG. 1 is a sectional view of a coreless motor showing an embodiment of the present invention. FIGS. 3 is a developed view showing a modified example of the winding pattern in the rotor, FIG. 4 is a cross-sectional view of the rotor showing another embodiment of the present invention, and FIGS. 5 and 6 are other embodiments of the rotor. 7(A) is a perspective view of a rotor in a coreless motor, and FIG. 7(B) is a cross-sectional view of a conductor wire showing an example. FIG. 7(B) is a diagram of a coreless motor to which the rotor shown in FIG. 7(^) is applied. The cross-sectional view, Figures 8 and 9 are one example of a conventional coreless motor.
FIG. l...rotating shaft, 2.9...conducting wire, 38...commutator, 3B...brush, 4...permanent magnet, 5...outer core, 6...current direction, 7... Rotation direction, 8... Rotor, 1-0... Superconducting thin film, 11A... Insulating adhesive, 11B... Resin, 13... Metal substrate, 14... Lines of magnetic force distribution. Figure 2 (A) Figure 2 (B) 3A 31st,, Knee 35 Figure 6 Figure 6 Den;

Claims (1)

【特許請求の範囲】 1)少なくとも1つの平面を有する金属基板と、 該金属基板が有する前記少なくとも1つの平面上に形成
された超伝導材薄膜と によって構成されることを特徴とする導線。 2)前記超伝導材薄膜が金属によって被覆されることを
特徴とする請求項1に記載の導線。 3)磁束発生手段を有し、前記超伝導材薄膜の膜面が前
記磁束の方向と平行になるよう請求項1または2に記載
の導線を配設したことを特徴とする電気機器。 4)固定子としての磁束発生手段を有し、回転子におけ
る電流路が請求項1または2に記載の導線によって構成
され、前記超伝導材薄膜の膜面が前記電流路を鎖交する
前記磁束の方向と平行であることを特徴とするコアレス
モータ。
Claims: 1) A conductive wire comprising: a metal substrate having at least one plane; and a superconducting thin film formed on the at least one plane of the metal substrate. 2) The conducting wire according to claim 1, wherein the superconducting thin film is coated with metal. 3) An electrical device comprising a magnetic flux generating means, wherein the conducting wire according to claim 1 or 2 is disposed such that the film surface of the superconducting material thin film is parallel to the direction of the magnetic flux. 4) The magnetic flux has a magnetic flux generating means as a stator, the current path in the rotor is constituted by the conducting wire according to claim 1 or 2, and the film surface of the superconducting material thin film interlinks the current path. A coreless motor characterized by being parallel to the direction of.
JP63081397A 1987-07-22 1988-04-04 Coreless motor Expired - Fee Related JP2746596B2 (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
JP63081397A JP2746596B2 (en) 1988-04-04 1988-04-04 Coreless motor
US07/220,162 US5099162A (en) 1987-07-22 1988-07-18 Coil of superconducting material for electric appliance and motor utilizing said coil
US08/138,389 US5389908A (en) 1987-07-22 1993-10-20 Coil of superconducting material for electric appliance and motor utilizing said coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63081397A JP2746596B2 (en) 1988-04-04 1988-04-04 Coreless motor

Publications (2)

Publication Number Publication Date
JPH01255451A true JPH01255451A (en) 1989-10-12
JP2746596B2 JP2746596B2 (en) 1998-05-06

Family

ID=13745172

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63081397A Expired - Fee Related JP2746596B2 (en) 1987-07-22 1988-04-04 Coreless motor

Country Status (1)

Country Link
JP (1) JP2746596B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP4395136A4 (en) * 2021-08-26 2025-07-30 Tdk Corp STATOR
JP7782472B2 (en) * 2022-02-24 2025-12-09 株式会社デンソー Coil body, armature and rotating electric machine
WO2023163136A1 (en) * 2022-02-24 2023-08-31 株式会社デンソー Coil body, armature, and rotary electric machine

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62277704A (en) * 1986-05-26 1987-12-02 Fujikura Ltd Manufacture of superconducting sheet coil
JPH01144345A (en) * 1987-11-27 1989-06-06 Mitsubishi Electric Corp Induction motor

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62277704A (en) * 1986-05-26 1987-12-02 Fujikura Ltd Manufacture of superconducting sheet coil
JPH01144345A (en) * 1987-11-27 1989-06-06 Mitsubishi Electric Corp Induction motor

Also Published As

Publication number Publication date
JP2746596B2 (en) 1998-05-06

Similar Documents

Publication Publication Date Title
US5099162A (en) Coil of superconducting material for electric appliance and motor utilizing said coil
KR100635170B1 (en) Superconducting Magnetic Coils
JP3566559B2 (en) Stator coil winding
US4255684A (en) Laminated motor stator structure with molded composite pole pieces
KR920702059A (en) Lightweight, high power mechanism
US3356877A (en) Electromechanical energy converter of the double air gap type
US3091715A (en) Axial airgap rotary machines
US20080054733A1 (en) Slotless Ac Induction Motor
US5722153A (en) Method for fabricating a split-loop armature coil for a motor
JP2746596B2 (en) Coreless motor
CN1426625A (en) Superconductive armature winding for electrical machine
US3440456A (en) Commutating arrangement for electric machines with superconducting armature coils
JP2006166692A (en) Parallel winding superconducting coil for synchronous machine
JPH01190256A (en) motor
JP2950905B2 (en) Motor stator and motor
JP3120626B2 (en) Oxide superconducting conductor
JPS6215803A (en) Superconductive coil
JPH06260335A (en) High temperature superconducting magnet
JP2883071B1 (en) Superconducting field winding conductor
JPS58130759A (en) Plane opposite type dc motor
SU1015473A1 (en) Two-coordinate electric machine
JPH1041127A (en) Split type coil
JPH06176924A (en) Superconducting magnet
CA1142567A (en) Motor stator structure
JPH058641Y2 (en)

Legal Events

Date Code Title Description
LAPS Cancellation because of no payment of annual fees