JPH0421301A - Non-contact current collecting system for superconducting magnetic levitation railroad - Google Patents

Non-contact current collecting system for superconducting magnetic levitation railroad

Info

Publication number
JPH0421301A
JPH0421301A JP12481390A JP12481390A JPH0421301A JP H0421301 A JPH0421301 A JP H0421301A JP 12481390 A JP12481390 A JP 12481390A JP 12481390 A JP12481390 A JP 12481390A JP H0421301 A JPH0421301 A JP H0421301A
Authority
JP
Japan
Prior art keywords
coil
superconducting
current collecting
levitation
coils
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
JP12481390A
Other languages
Japanese (ja)
Other versions
JP2565582B2 (en
Inventor
Masayuki Shibata
将之 柴田
Naoki Maki
牧 直樹
Toshio Saito
敏雄 斉藤
Koji Kobayashi
孝司 小林
Eiji Sawano
澤野 英二
Hiroshi Oshima
浩 大島
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.)
Hitachi Ltd
Central Japan Railway Co
Original Assignee
Hitachi Ltd
Central Japan Railway Co
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 Hitachi Ltd, Central Japan Railway Co filed Critical Hitachi Ltd
Priority to JP2124813A priority Critical patent/JP2565582B2/en
Publication of JPH0421301A publication Critical patent/JPH0421301A/en
Application granted granted Critical
Publication of JP2565582B2 publication Critical patent/JP2565582B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Current-Collector Devices For Electrically Propelled Vehicles (AREA)
  • Control Of Vehicles With Linear Motors And Vehicles That Are Magnetically Levitated (AREA)

Abstract

PURPOSE:To enhance current collecting capacity and efficiency of a current collecting system and to facilitate manufacture of coil by forming circular or elliptical superconducting coils and current collecting coils and arranging upper and lower coils in 8-shape with different polarities. CONSTITUTION:Superconducting current collecting coils 6a, 6b and current collecting coils 7a-7f are connected in 8-shape similarly to levitation coils 4a-4f. Furthermore, the superconducting current collecting coils 6a, 6b are arranged with different polarities. The superconducting current collecting coils 6a-6d are formed into circular shape or elliptical shape. Pole pitch of the coils 6a-6d is set shorter than that of levitation/thrust superconducting coil.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は超電導磁気浮上方式鉄道用非接触集電システム
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a superconducting magnetic levitation non-contact current collection system for railways.

〔従来の技術〕[Conventional technology]

超電導磁石を用いた磁気浮上鉄道は第12図(a)に示
されているように、浮上・推進用超電導コイル1a、1
bを搭載した車体2を、地上に設置した推進コイル3a
、3b、3c、(3d。
As shown in Fig. 12(a), a magnetic levitation railway using superconducting magnets has superconducting coils 1a, 1 for levitation and propulsion.
Propulsion coil 3a installed on the ground
, 3b, 3c, (3d.

3e、3f)に、縦軸に電流をとり、横軸に時間をとっ
て示した第10図に示されているような3相の正弦波の
電流を与えることにより生ずる移動磁界によって推進さ
せる。また浮上はそれとは別のコイル間を8の字状に接
続して形成された8字の形をした浮上コイル4a、4b
、4c、4d、4e、4fに、第12図(b>に示され
ている矢印のように、誘起される反発磁束による力を利
用することによってなされるもので、供給される正弦波
の周波数を変化させることにより、始動から最終的には
約500km/時の超高速まで達することができる。な
お同図において5はガイドウェイである。
3e, 3f) are propelled by a moving magnetic field generated by applying a three-phase sinusoidal current as shown in FIG. 10, where the vertical axis represents the current and the horizontal axis represents time. In addition, the levitation coils 4a and 4b are formed by connecting other coils in a figure 8 shape.
, 4c, 4d, 4e, and 4f, as shown by the arrows in Figure 12 (b>), this is done by utilizing the force due to the induced repulsive magnetic flux, and the frequency of the supplied sine wave By changing the speed, it is possible to finally reach a super high speed of about 500 km/hour from start-up.In the figure, 5 is a guideway.

超電導磁気浮上システムでは車上用補助電源システムと
して、地上コイルに誘起される移動磁界のうち余分な成
分である高調波を利用した非接触集電システムが考えら
れている。しかしこの高調波の含まれている割合は地上
コイルの配置により異なり、場合によっては十分な電力
がとれないことも考えられる。そのため集電の目的のた
めに超電導コイルを車上に搭載することが、例えば第1
3図(a)、(b)に示されているように提案されてい
る。これは同図(a)に示されているように、集電用超
電導コイル6b、6dおよび集電コイル7a、7c、7
eが夫々車体の長手方向に沿って1列に配置されている
。この車上に搭載した集電用超電導コイル6b、6cl
が車両とともに移動することによって生ずる磁束変化に
よって、同図(b)の矢印のように地上の浮上コイル4
b、4d、(4f、浮上コイルの下部)に起電力が生じ
、8字に接続された浮上コイル4a、4c、(4e、浮
上コイルの上部)に電流が流れることにより生成された
磁束を、車上の集電コイル7a、7c、7eによってひ
ろいあげることにより、集電するものである。
In the superconducting magnetic levitation system, a non-contact current collection system that uses harmonics, which are extra components of the moving magnetic field induced in the ground coil, is being considered as an on-board auxiliary power supply system. However, the proportion of harmonics included varies depending on the arrangement of the ground coils, and in some cases it may not be possible to obtain sufficient power. Therefore, it is important to install a superconducting coil on the vehicle for the purpose of current collection, for example, in the first
It is proposed as shown in Figure 3 (a) and (b). As shown in FIG.
e are arranged in one row along the longitudinal direction of the vehicle body. Superconducting coils 6b and 6cl for current collection mounted on this vehicle
Due to changes in magnetic flux caused by the movement of the coil 4 with the vehicle, the levitation coil 4 on the ground is
Electromotive force is generated in b, 4d, (4f, lower part of the levitation coil), and the magnetic flux generated by current flowing through the levitation coils 4a, 4c, (4e, upper part of the levitation coil) connected in a figure 8, Current is collected by spreading it through current collecting coils 7a, 7c, and 7e on the vehicle.

なお、この種システムに関するものに、対向浮上方式の
場合の非接触集電方式、例えば特開昭54−1’572
05号公報がある。
Regarding this type of system, there is a non-contact current collection method in the case of a counter-levitation method, for example, Japanese Patent Application Laid-Open No. 54-1'572.
There is a publication No. 05.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記従来技術では集電用超電導コイルと集電コイルとが
上下に夫々1列に配置されるので1発生する磁束量が少
なくて集電の力が小さい欠点があった。また超電導磁石
は人体または他の機械への悪影響をなくすため磁気シー
ルドが必要であるが。
In the above-mentioned conventional technology, since the superconducting coil for current collection and the current collecting coil are arranged in one row above and below, there is a drawback that the amount of magnetic flux generated is small and the current collecting force is small. Additionally, superconducting magnets require magnetic shielding to eliminate any negative effects on the human body or other machines.

列車の進行方向に必要な空間を多くとらなければならず
、はなはだ不経済であった。
This required a large amount of space in the direction of train travel, which was extremely uneconomical.

本発明は以上の点に鑑みなされたものであり、集電能力
の向上を可能としだ集電システムを提供すること。
The present invention has been made in view of the above points, and an object of the present invention is to provide a current collection system that can improve current collection ability.

集電効率の向上を可能とした集電システムを提供するこ
と。
To provide a current collection system that can improve current collection efficiency.

製作を容易にすることを可能とした集電用超電導コイル
および集電コイルを提供すること。
To provide a superconducting coil for current collection and a current collection coil that can be manufactured easily.

保守、点検を容易にすることを可能としだ集電用超電導
コイルおよび集電コイルを提供すること。
To provide a superconducting coil for current collection and a current collection coil that enable easy maintenance and inspection.

浮上特性に悪影響を及ぼさないようにすることを可能と
しだ集電用超電導コイルを提供すること。
To provide a superconducting coil for current collection that can prevent levitation characteristics from being adversely affected.

車両の空間を有効に利用することを可能としだ集電シス
テムを提供すること。
To provide a current collection system that enables effective use of space in a vehicle.

を目的とするものである。The purpose is to

〔課題を解決するための手段〕[Means to solve the problem]

集電能力の向上を可能としだ集電システムを提供するの
に、集電用超電導コイルおよび集電コイルを、浮上コイ
ルのそれと同じようにその上下に配置したコイル間を8
の字状に接続してなる8字形形状とした。また、集電用
超電導コイルおよび集電コイルを、その上下に配置した
コイルが夫々異なる極を有している異極配置とした。
In order to provide a current collection system that can improve the current collection capacity, the superconducting coil for current collection and the current collection coil are placed above and below each other in the same way as the levitation coil.
It has a figure 8 shape connected in a figure shape. Further, the current collecting superconducting coil and the current collecting coil were arranged in a different polarity arrangement in which the coils disposed above and below each have different poles.

集電効率の向上を可能としだ集電システムを提供するの
に、集電用超電導コイルのポールピッチを、浮上・推進
用超電導コイルのポールピッチより小さくした。
In order to provide a current collection system that can improve current collection efficiency, the pole pitch of the current collection superconducting coil was made smaller than the pole pitch of the levitation/propulsion superconducting coil.

製作を容易にすることを可能としだ集電用超電導コイル
および集電コイルを提供するのに、集電用超電導コイル
および集電コイルを1円形状または楕円状に形成した。
In order to provide a superconducting current collecting coil and a current collecting coil that can be manufactured easily, the superconducting current collecting coil and the current collecting coil are formed into a circular shape or an elliptical shape.

保守1点検を容易にすることを可能としだ集電用超電導
コイルおよび集電コイルを提供するのに、集電用超電導
コイルおよび集電コイルを、特定の車両に搭載した。
In order to provide a superconducting current collecting coil and a current collecting coil that can facilitate maintenance and inspection, the superconducting current collecting coil and current collecting coil are mounted on a specific vehicle.

浮上特性に悪影響を及ぼさないようにすることを可能と
しだ集電用超電導コイルを提供するのに、集電用超電導
コイルおよび集電コイルを、その上下に配置されたコイ
ル間の距離を浮上コイルの上下間の距離よりも大きくし
た。また、集電用超電導コイルおよび集電コイルを、昇
降装置で上下に移動自在に形成した。
In order to provide a superconducting coil for current collection that does not adversely affect the levitation characteristics, the superconducting coil for current collection and the distance between the coils placed above and below the levitation coil must be adjusted. greater than the distance between the top and bottom of. In addition, the current collecting superconducting coil and the current collecting coil were formed to be movable up and down using a lifting device.

車両の空間を有効に利用することを可能としだ集電シス
テムを提供するのに、集電用超電導コイルを、同一の極
低温容器に牧納した。
In order to provide a current collection system that makes effective use of vehicle space, the superconducting coils for current collection are housed in the same cryogenic container.

〔作用〕[Effect]

集電用超電導コイルおよび集電コイルを、浮上コイルの
それと同じようにその上下に配置したコイル間を8の字
状に接続してなる8字形形状とした。また。その上下に
配置したコイルが夫々異なる極を有している異極配置と
したので、浮上コイルに流れる電流が従来に比べて約2
倍になって、車上の集電コイルに誘起される電圧が約2
倍となる。
The superconducting coil for current collection and the current collecting coil have a figure-8 shape in which the coils arranged above and below are connected in a figure-8 shape in the same way as the levitation coil. Also. Since the coils placed above and below the levitation coil have different polarity, the current flowing through the levitation coil is approximately 2
This increases the voltage induced in the current collector coil on the vehicle by approximately 2
It will be doubled.

集電用超電導コイルのポールピッチを、浮上・推進用超
電導コイルのポールピッチより小さくしたので、次数の
少ない高調波を利用することができるようになって、振
幅の大きい磁束が利用できるようになる。
The pole pitch of the superconducting coil for current collection is made smaller than the pole pitch of the superconducting coil for levitation and propulsion, making it possible to use harmonics with a small number of orders, making it possible to use magnetic flux with a large amplitude. .

集電用超電導コイルおよび集電コイルを円形状または楕
円状に形成したので、集電用超電導コイルおよび集電コ
イルが作り易くなる。
Since the current collecting superconducting coil and the current collecting coil are formed in a circular or elliptical shape, the current collecting superconducting coil and the current collecting coil can be easily manufactured.

集電用超電導コイルおよび集電コイルを特定の車両に搭
載したので、特定の車両のみ保守1点検すればよくなる
Since the current collecting superconducting coil and the current collecting coil are mounted on a specific vehicle, it is only necessary to perform one maintenance inspection on the specific vehicle.

集電用超電導コイルおよび集電コイルを、その上下に配
置されたコイル間の距離を夫々浮上コイルの上下間の距
離よりも大きくしたので5車体の上下変動時でも上向き
の力が存在するようになって、浮上特性の平衡特性が保
たれるようになる。
The distance between the superconducting coils for current collection and the current collecting coils placed above and below them was made larger than the distance between the top and bottom of the levitation coils, so that an upward force is present even when the vehicle body moves up and down. As a result, the balanced characteristics of the flying characteristics are maintained.

集電用超電導コイルを同一の極低温容器に敗納したので
、異極配置時の集電用超電導コイルも同一のクライオス
タット内に配置されるようになる。
Since the current collecting superconducting coils are stored in the same cryogenic container, the current collecting superconducting coils when different poles are arranged are also placed in the same cryostat.

〔実施例〕〔Example〕

以下1図示した実施例に基づいて本発明を説明する。第
1図(a)、(b)には本発明の−実施例が示されてい
る。なお従来と同し部品には同じ符号を付したので説明
を省略する。本実施例では集電用超電導コイル6a、6
b、・・・および集電コイル7a、7b、7c、7d、
7e、7 f ・・・を、浮上コイル4a、4b、4C
14d、4e、4f・・・のそれと同じようにその上下
に配置したコイル(6a、6b)、(7a、7b・)間
を8の字状に接続してなる8字形形状とした。このよう
にすることにより浮上コイル4a、4b、4c、4d、
4e、4f・・・に流れる電流Iが従来に比べ約2倍と
なって、−車上の集電コイル7a、7b、7C17d、
7e、7f・・・に誘起される電圧が約2倍となり、集
電能力の向上を可能としだ集電システムを得ることがで
きる。
The present invention will be explained below based on an embodiment shown in one figure. An embodiment of the invention is shown in FIGS. 1(a) and 1(b). Note that parts that are the same as those in the prior art are designated by the same reference numerals, and therefore their explanations will be omitted. In this embodiment, superconducting coils 6a, 6
b, ... and current collecting coils 7a, 7b, 7c, 7d,
7e, 7f..., levitation coils 4a, 4b, 4C
Similar to those of 14d, 4e, 4f, etc., the coils (6a, 6b) and (7a, 7b) arranged above and below are connected in a figure 8 shape to form a figure 8 shape. By doing this, the levitation coils 4a, 4b, 4c, 4d,
The current I flowing through 4e, 4f, etc. is about twice as much as that of the conventional one, and - the current collecting coils 7a, 7b, 7C17d on the vehicle,
The voltage induced in 7e, 7f, . . . is approximately doubled, making it possible to obtain a current collection system with improved current collection ability.

すなわち車上に搭載された集電用超電導コイル6a、6
b・・は8字形に接続されている。この集電用超電導コ
イル6a、6b・・を搭載した車両が例えば500km
/時で走行すると、電磁誘導により地上に設置された8
字状に接続してなる8字形をした浮上コイル4a、4b
、4C14d、4e、4f・・に第10図に示されてい
るように、3相の正弦波状の電流が流れる。この3相の
正弦波状電流の作る集電コイル7a、7b、7c、7d
、7e、7f・・・の位置における磁場の分布は、第1
1図(a)、(b)、(c)、に示されているように、
同図(a)記載の磁場には同図(b)の列車と共に進む
基本波の他にさらに同図(c)に記載されているように
、周波数の高い高調波(第2次空間高調波)が含まれて
いる。基本波は列車と共に進むので列車側からは単に直
流成分にしかならないが、高調波成分は列車の数倍の速
さで進むので、上述のようにこの成分を利用して集電能
力を得ることができる。この高調波磁場を取り出すのが
車上に設置された集電コイル7a、7b、7c、7d、
7e、7 f−・であり、これも8字形に接続されてい
る。従って集電コイル7a、7b。
In other words, the current collecting superconducting coils 6a, 6 mounted on the vehicle
b... are connected in a figure 8 pattern. A vehicle equipped with these superconducting coils 6a, 6b, etc. for current collection is, for example, 500 km.
When traveling at / hour, 8 installed on the ground by electromagnetic induction
8-shaped levitation coils 4a and 4b connected in a figure-like shape
, 4C14d, 4e, 4f, . . . as shown in FIG. 10, three-phase sinusoidal currents flow. Current collector coils 7a, 7b, 7c, 7d created by these three-phase sinusoidal currents
, 7e, 7f... The distribution of the magnetic field at the positions of the first
As shown in Figures 1 (a), (b), and (c),
In addition to the fundamental wave that travels with the train as shown in (b), the magnetic field shown in (a) of the same figure contains high-frequency harmonics (secondary spatial harmonics) as shown in (c) of the same figure. )It is included. The fundamental wave travels with the train, so from the train side it simply becomes a DC component, but the harmonic component travels several times faster than the train, so as mentioned above, this component can be used to obtain current collection ability. I can do it. The collector coils 7a, 7b, 7c, 7d installed on the vehicle extract this harmonic magnetic field.
7e, 7f-・, which are also connected in a figure-eight pattern. Therefore, current collecting coils 7a, 7b.

7c、7d、7e、7f・・・の数が従来に比べて同じ
長手方向長さあたり2倍となり、夫々の電圧も約2倍と
なり、取り出される磁束も同じ長手方向長さあたり約5
〜8倍となる。この集電コイル7a、7b、7c、7d
、7e、7fは第14図に示されているように、コンバ
ータ8、バッファ用蓄電池9、更にインバータ10に接
続され、最終的に負荷11に接続される。なお第1図(
b)において12は車輪である。
The number of 7c, 7d, 7e, 7f... is doubled per the same longitudinal length compared to the conventional one, the voltage of each is also about twice, and the magnetic flux taken out is also about 5 per the same longitudinal length.
~8 times. These current collecting coils 7a, 7b, 7c, 7d
, 7e, and 7f are connected to a converter 8, a buffer storage battery 9, an inverter 10, and finally a load 11, as shown in FIG. In addition, Figure 1 (
In b), 12 is a wheel.

第2図には本発明の他の実施例が示されている。Another embodiment of the invention is shown in FIG.

本実施例は集電用超電導コイル6a、6b・・・を。In this embodiment, superconducting coils 6a, 6b, . . . for collecting current are used.

その上下に配置したコイル(6a、6b)が夫々異なる
極を有している異極配置とした。このようにすることに
より、集電用超電導コイル6a、6b・・に流れる電流
工が、第1図のそれと同しように、上下のコイル6a、
6b間で反対方向に流れるようになって、浮上コイル4
a〜4fに流れる電流が従来に比べて約2倍となり、前
述の場合と同様な作用効果を奏することができる。
The coils (6a, 6b) disposed above and below were arranged in a different polarity arrangement, each having a different pole. By doing this, the electric current flowing through the current collecting superconducting coils 6a, 6b, etc. can be changed to the upper and lower coils 6a, 6b, etc., as shown in FIG.
6b in the opposite direction, the levitation coil 4
The current flowing through a to 4f is approximately twice that of the conventional case, and the same effects as in the case described above can be achieved.

第3図には以上の実施例でどの程度の集電が可能かどう
かの検討を行った結果が示されている。
FIG. 3 shows the results of a study on how much current can be collected in the above embodiment.

これは同図記載の数値、浮上コイル(8字1ターン)4
a、4bの自己インダクタンス(L)0゜98μH1抵
抗(R)33.8μΩ、集電コイル(8字3ターン)7
a、7b・・の自己インダクタンス(L)6.66μH
1抵抗(R)437μΩ、集電用超電導コイル6a、・
・・の幅0.60m、高さ0.34m、集電コイル7a
、・・・の幅0.175m、高さ0.34m、浮上コイ
ル4a、・・・の幅0.35m、高さQ、34m等を用
いて検討したものである。集電用超電導コイル6a、・
・に3゜0kATのDC電流を流すと、地上の浮上コイ
ル4a、・・・には実効値で42kAT、102.9H
zのAC電流が流れる(500km/時)。このAC電
流の作る磁束によって誘起される車上の集電コイル7a
、・・・1ターンあたりの起電力は第2次空間高調波(
第2次空間高調波は時間的には3次となる)を利用する
ので、実効値7.4V、308゜7臣となる。同図(a
)の装置を先頭車両と後尾車両の左右に、列車進行方向
に5.4mの長さ設置すると、1車両あたり3相線間電
圧600V、最大で408kW(1編成ではその2倍の
816kW)の電力がとれる(同図(c)参照)。
This is the value shown in the same figure, levitation coil (8 characters 1 turn) 4
Self-inductance (L) of a, 4b 0゜98μH1 Resistance (R) 33.8μΩ, current collector coil (8 characters 3 turns) 7
Self-inductance (L) of a, 7b...6.66μH
1 resistance (R) 437 μΩ, current collecting superconducting coil 6a,
...width 0.60m, height 0.34m, current collector coil 7a
, . . . width 0.175 m, height 0.34 m, levitation coil 4a, . . . width 0.35 m, height Q, 34 m, etc. Superconducting coil 6a for current collection,
When a DC current of 3°0kAT is applied to the levitation coil 4a on the ground, the effective value is 42kAT, 102.9H.
An AC current of z flows (500 km/hour). The current collector coil 7a on the vehicle is induced by the magnetic flux created by this AC current.
,...The electromotive force per turn is the second spatial harmonic (
Since the second-order spatial harmonic is the third-order in terms of time), the effective value is 7.4V and 308°7. The same figure (a
) is installed on the left and right sides of the leading car and the trailing car for a length of 5.4 m in the direction of train movement, the voltage between the three-phase lines per car is 600 V, and the maximum is 408 kW (816 kW, twice that for one train). Electricity can be obtained (see figure (c)).

第4図には本発明の更に他の実施例が示されている。本
実施例では集電用超電導コイル6a、6b、6c、6d
のポールピッチP1を、浮上・推進用超電導コイルla
、lbのポールピッチP2より小さくした。このように
することにより次数の少ない高調波を利用することがで
きるようになって、振幅の大きい磁束が利用できるよう
になり、集電システムの集電効率を向上させることがで
きる。
FIG. 4 shows yet another embodiment of the invention. In this embodiment, current collecting superconducting coils 6a, 6b, 6c, 6d
The pole pitch P1 of levitation/propulsion superconducting coil la
, lb pole pitch P2. By doing so, harmonics with a small number of orders can be used, magnetic flux with a large amplitude can be used, and the current collection efficiency of the current collection system can be improved.

すなわち集電用超電導コイル6a、6b、6c、6dの
ポールピッチP工を浮上・推進用超電導コイル1a、1
bのポールピッチP2のそれぞれ1/2にした。集電用
超電導コイル6a、6b、6c、6dのポールピッチP
1が浮上・推進用超電導コイル1a、1bのポールピッ
トP2と同じ場合は第11図(d)、(e)、(f)に
見られるように、集電コイル位置に見られる磁場分布は
、基本波(同図(e)参照)に第5次空間高調波(第5
次高調波)が乗っているものである(同図(f)参照)
、これに対してポールピッチが1/2の場合は前述の第
11図(a)、(b)、(c)に見られるように基本波
(同図(b)参照)に第2次空間高調波が乗るもの(同
図(c)参照)で、振幅が第11図(f)のそれよりも
大きい。従ってこの大きい振幅を利用するので、ポール
ピッチが同じ場合に比べて非接触集電能力が増大する。
That is, the pole pitch P of the superconducting coils 6a, 6b, 6c, and 6d for current collection is the superconducting coil for levitation and propulsion 1a, 1.
The pole pitch P2 of b is set to 1/2. Pole pitch P of superconducting coils 6a, 6b, 6c, 6d for current collection
1 is the same as the pole pit P2 of the superconducting coils 1a and 1b for levitation and propulsion, the magnetic field distribution seen at the current collecting coil position is as shown in FIGS. 11(d), (e), and (f). The fundamental wave (see (e) in the same figure) and the 5th spatial harmonic (5th
(see figure (f))
On the other hand, when the pole pitch is 1/2, the fundamental wave (see figure 11(b)) has a secondary space, as seen in Figure 11 (a), (b), and (c). This is the one on which harmonics are carried (see Figure 11(c)), and the amplitude is larger than that in Figure 11(f). Therefore, since this large amplitude is utilized, the non-contact current collection ability is increased compared to the case where the pole pitch is the same.

なお第11図(d)は同図の(e)、(f)を合成した
磁場の変化を示したものである。
Note that FIG. 11(d) shows a change in the magnetic field obtained by combining (e) and (f) in the same figure.

第5図(a)、(b)には本発明の更に他の実施例が示
されている。本実施例は集電用超電導コイル6a、6b
、6c、6dの形状をそれぞれ円形(同図(a)参照)
、楕円形(同図(b)参照)にしたものである。このよ
うにすることにより円形または楕円形なので集電用超電
導コイル6a、6b、6c、6dの製作を容易にするこ
とができる。なお、本実施例では集電用超電導コイル6
a、6b、6c、6dを円形状または楕円状に形成した
場合について述べたが、集電コイルについても同様に実
施し、同様の効果をあくることかできる。
Still another embodiment of the present invention is shown in FIGS. 5(a) and 5(b). In this embodiment, superconducting coils 6a and 6b for current collection are used.
, 6c, and 6d are circular (see figure (a)).
, and has an elliptical shape (see (b) in the same figure). By doing so, the current collecting superconducting coils 6a, 6b, 6c, and 6d can be easily manufactured because they are circular or elliptical. In addition, in this embodiment, the current collecting superconducting coil 6
Although the case where a, 6b, 6c, and 6d are formed in a circular or elliptical shape has been described, the same can be applied to the current collecting coil to achieve the same effect.

第6図には本発明の更に他の実施例が示されている。本
実施例は集電用超電導コイル6a、6b、6c、6dを
特定の車両に搭載した。すなわち集電用超電導コイル6
a、6b、6c、6dを1例えば先頭車両または後尾車
両に集中して配置するようにした。このようにすること
により先頭車両または後尾車両を点検すればよくなって
、集電用超電導コイル6a、6b、6c、6dの保守点
検を容易にすることができる。なお、この場合、その車
両を集電のみを目的とした専用車両とすることも含む。
FIG. 6 shows yet another embodiment of the invention. In this embodiment, current collecting superconducting coils 6a, 6b, 6c, and 6d are mounted on a specific vehicle. In other words, the superconducting coil 6 for current collection
a, 6b, 6c, and 6d are arranged in a concentrated manner, for example, in the leading vehicle or the trailing vehicle. By doing so, it is only necessary to inspect the leading vehicle or the trailing vehicle, and maintenance and inspection of the current collecting superconducting coils 6a, 6b, 6c, and 6d can be facilitated. Note that in this case, the vehicle may also be a dedicated vehicle for the sole purpose of collecting current.

なおまた、本実施例では集電用超電導コイル6a、6b
、6c、6dにツいて述べたが。
Furthermore, in this embodiment, the current collecting superconducting coils 6a, 6b
, 6c, and 6d.

集電コイルについても同様に実施することができる。The same can be applied to the current collecting coil.

第8図(a)、(b)には本発明の更に他の実施例が示
されている。本実施例では集電用超電導コイル6a、6
b・・・の上下に配置されたコイル(6a、6b)間の
距離を、浮上コイル4a、4bの上下間の距離よりも大
きくした。このようにすることにより車体の上下変動時
でも上向きの力が存在するようになって、浮上特性の平
衡特性が保たれるようになり、集電用超電導コイル6a
、6b・・・の浮上特性に悪影響を及ぼすのを防止する
ことができる。
Still another embodiment of the present invention is shown in FIGS. 8(a) and 8(b). In this embodiment, superconducting coils 6a, 6
The distance between the coils (6a, 6b) placed above and below b... was made larger than the distance between the top and bottom of the levitation coils 4a, 4b. By doing this, an upward force is present even when the vehicle body moves up and down, and the balanced characteristics of the levitation characteristics are maintained, and the current collecting superconducting coil 6a
, 6b, . . . can be prevented from having an adverse effect on the flying characteristics.

すなわち第1図(b)のように、集電用超電導コイル6
a、6bと浮上コイル4a、4bとの上下のコイル配置
が等しい場合では、主に加速、減速時の低速走行時にお
いて、集電用超電導コイル6a、6bの中心位置が浮上
コイル4a、4bのそれよりも下にずれた場合、第7図
に示されているように図中矢印表示の下向きのカだけが
働くので、集電用超電導コイル6a、6bが浮上特性に
悪影響を及ぼす。この場合は例えば第8図(a)のよう
に、集電用超電導コイル6a、6bの上下の距離、すな
わち6a、6b間の距離を浮上コイル4a、4bのそれ
より離して配置することにより、中心位置の一致する定
速走行時のみならず、加速時または減速時においてその
中心位置が下側にずれた場合にも、集電用超電導コイル
6a、6bの上部のコイル6aが浮上コイル4a、4b
の上部のコイル4aより上に位置するようになって、上
向きの力が働き、浮上刃に悪影響を及ぼさないようにす
ることができる。
That is, as shown in FIG. 1(b), the current collecting superconducting coil 6
If the upper and lower coil arrangements of a and 6b and the levitation coils 4a and 4b are the same, the center position of the current collecting superconducting coils 6a and 6b will be the same as that of the levitation coils 4a and 4b, mainly during low-speed running during acceleration and deceleration. If the current-collecting superconducting coils 6a and 6b are shifted downwards, only the downward force shown by the arrow in the figure acts, as shown in FIG. In this case, for example, as shown in FIG. 8(a), by arranging the distance between the top and bottom of the current collecting superconducting coils 6a and 6b, that is, the distance between 6a and 6b, from that of the levitation coils 4a and 4b, Not only during constant speed travel when the center positions match, but also when the center positions shift downward during acceleration or deceleration, the upper coil 6a of the current collecting superconducting coils 6a, 6b is activated by the levitation coil 4a, 4b
Since the floating blade is located above the upper coil 4a, an upward force is exerted to prevent the floating blade from being adversely affected.

また第8図(b)のように、列車の浮上位置を検出する
検品装置13を設け、さらにその検出された位置に従っ
て集電用超電導コイル6a、6bおよび集電コイル7a
、7bを昇降させる昇降装M14を設けることにより、
あらゆる速度におし)で前述の場合と同様な作用効果を
奏することができる。
In addition, as shown in FIG. 8(b), an inspection device 13 is provided to detect the floating position of the train, and according to the detected position, the current collecting superconducting coils 6a, 6b and the current collecting coil 7a are
, 7b, by providing an elevator M14 for raising and lowering the
The same effects as those described above can be achieved at any speed.

第9図は本発明の更に他の実施例を示すもので。FIG. 9 shows still another embodiment of the present invention.

集電用超電導コイル6a、6bを8の字に接続した場合
のみならず、そうでない場合(異極配置)でも同じクラ
イオスタット15に入れたものである。このようにする
ことにより、列車の空間を有効に利用することができる
The current collecting superconducting coils 6a and 6b are placed in the same cryostat 15 not only when they are connected in a figure 8 configuration, but also when they are not connected in a figure 8 configuration (different polarity arrangement). By doing so, the space on the train can be used effectively.

以上述べてきた実施例によれば次に述べるような効果を
奏することができる。
According to the embodiments described above, the following effects can be achieved.

(1)集電用超電導コイルおよび集電コイルを8字、ま
たはそれと同等の機能を持つように異極配置し、さらに
上下2重に配電したので集電の能力が増大し、また列車
の進行方向に必要な磁気シールドのための空間を少なく
することができる。
(1) The superconducting coil for current collection and the current collecting coil are arranged with different polarities to have a figure 8 or equivalent function, and the power is distributed in two layers above and below, which increases current collection ability and improves train progress. The space required for magnetic shielding in this direction can be reduced.

(2)集電用超電導コイルのポールピッチを浮上・推進
用コイルのそれより小さくした、例えば1/2にするこ
とにより、効率の向上を可能とした集電が可能になる。
(2) By making the pole pitch of the current collection superconducting coil smaller than that of the levitation/propulsion coil, for example, 1/2, current collection with improved efficiency becomes possible.

(3)集電用超電導コイルおよび集電コイルを円形また
は楕円形にすることにより、これらコイルの製作を容易
にすることができる。
(3) By making the current collecting superconducting coil and current collecting coil circular or elliptical, manufacturing of these coils can be facilitated.

(4)集電用超電導コイルおよび集電コイルを特定の車
両に搭載することにより、集電システムの保守1点検を
容易にすることができる。
(4) By mounting the current collecting superconducting coil and the current collecting coil on a specific vehicle, maintenance and inspection of the current collecting system can be facilitated.

(5)集電用超電導コイルおよび集電コイルの上下間距
離を浮上コイルの上下間距離より離すことにより、また
集電用超電導コイルおよび集電コイルを上下に移動させ
る昇降装置を設置することにより、磁気浮上列車の浮上
刃に悪影響を及ぼさないようにできる。
(5) By making the superconducting coil for current collection and the distance between the top and bottom of the current collecting coil greater than the distance between the top and bottom of the levitation coil, and by installing a lifting device that moves the superconducting coil for current collection and the current collecting coil up and down. , it is possible to avoid having a negative effect on the levitation blades of the magnetic levitation train.

(6)上下の集電用超電導コイルを同一のクライオスタ
ットに敗納することにより、同一のクライオスタットに
牧納しない場合に比べて空間を有効に利用することがで
きる。
(6) By housing the upper and lower current collecting superconducting coils in the same cryostat, space can be used more effectively than when they are not housed in the same cryostat.

〔発明の効果〕〔Effect of the invention〕

上述のように本発明は、次に述べる効果を奏することが
できる。
As described above, the present invention can produce the following effects.

集電システムの集電能力が向上するようになって、集電
能力の向上を可能としだ集電システムを得ることができ
る。
Since the current collection ability of the current collection system is improved, a current collection system that can improve the current collection ability can be obtained.

集電システムの集電効率が向上するようになって、集電
効率の向上を可能としだ集電システムを得ることができ
る。
The current collection efficiency of the current collection system is improved, and a current collection system capable of improving the current collection efficiency can be obtained.

集電用超電導コイルおよび集電コイルの製作が容易とな
って、製作を容易にすることを可能とした集電用超電導
コイルおよび集電コイルを得ることができる。
The superconducting coil for current collection and the current collecting coil can be manufactured easily, and the superconducting coil for current collecting and the current collecting coil that can be manufactured easily can be obtained.

集電用超電導コイルおよび集電コイルの保守、点検が容
易となって、保守、点検を容易にすることを可能としだ
集電用超電導コイルおよび集電コイルを得ることができ
る。
The superconducting coil for current collection and the current collecting coil can be easily maintained and inspected, and the superconducting coil for current collecting and the current collecting coil that can be easily maintained and inspected can be obtained.

集電用超電源コイルを浮上特性に悪影響を及ぼさないよ
うにすることができるようになって、浮上特性に悪影響
を及ぼさないようにすることを可能としだ集電用超電導
コイルを得ることができる。
It has become possible to make the superpower coil for current collection so that it does not adversely affect the levitation characteristics, and it is now possible to obtain a superconducting coil for current collection that can be made so that the levitation characteristics are not adversely affected. .

集電システムは車両の空間を有効に利用できるようにな
って、車両の空間を有効に利用することを可能としだ集
電システムを得ることができる。
The current collection system can effectively utilize the space of the vehicle, and a current collection system that can effectively utilize the space of the vehicle can be obtained.

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

第1図(a)、(b)は本発明の超電導磁気浮上方式鉄
道用非接触集電システムの一実施例の集電用超電導コイ
ル、集電コイル、浮上コイルの配置を示すもので(a)
は進行方向と垂直な方向から見た説明図、(b)は進行
方向と同じ方向から見た説明図、第2図は本発明の超電
導磁気浮上方式鉄道用非接触集電システムの他の実施例
の進行方向と垂直な方向から見た集電用超電導コイル、
集電コイル、浮上コイルの配置を示す説明図、第3図(
a)、(b)、(c)は第1図5第2図による集電の効
果を検討するもので、(a)は集電用超電導コイル、集
電コイル、浮上コイルの夫々の所要寸法を示す説明図、
(b)は集電用超電導コイル、集電コイル、浮上コイル
間の寸法を示す説明図、(c)は発生電圧を示す説明図
、第4図は本発明の超電導磁気浮上方式鉄道用非接触集
電システムの更に他の実施例の浮上・推進用超電導コイ
ル、集電用超電導コイルのポールピッチの大きさを示す
説明図、第5図(a)、(b)は本発明の超電導磁気浮
上方式鉄道用非接触集電システムの更に他の実施例の集
電用超電導コイルの形状を示すもので、(a)は円形状
、(b)は楕円状に形成した場合の説明図、第6図は本
発明の超電導磁気浮上方式鉄道用非接触集電システムの
更に他の実施例の集電用超電導コイルの配置を示す説明
図、第7図は集電用超電導コイルが浮上特性に悪影響を
及ぼす状態を示す説明図、第8図(a)、(b)は本発
明の超電導磁気浮上方式鉄道用非接触集電システムの更
に他の実施例の浮上特性に悪影響に及ぼさない集電用超
電導コイルおよび集電コイルの配置を示すもので、(a
)はこれら両コイル間の夫々の距離を浮上コイルの上下
間距離より離した場合を示す説明図、(b)は集電用超
電導コイルおよび集電コイルに昇降装置を設けた場合を
示す説明図、第9図は本発明の超電導磁気浮上方式鉄道
用非接触集電システムの更に他の実施例の異極配置の集
電用超電導コイルをクライオスタット内に敗納した状態
を示す説明図、第10図は集電用超電導コイルによって
浮上コイルに誘起される3相の正弦波状電流の波形図、
第11図(a)〜(f)は浮上コイルに誘起される正弦
波状電流によって集電コイルの位置に生成される磁場分
布を示すもので、(a)〜(c)は集電用超電導コイル
のポールピッチが浮上・推進用超電導コイルの172の
場合で(a)は合成波、(b)基本波、(c)は第2次
空間高調波の波形図。 (d)〜(f)は集電用超電導コイルのポールピッチが
浮上・推進用超電導コイルのポールピッチと同じ場合で
(cl)は合成波、(e)は基本波、(f)は第5次空
間高調波の波形図、第12図(a)、(b)は従来の磁
気浮上列車の基本的な動きを説明するもので、(a)は
各種コイルの配置を列車進行方向の横から見た状態を示
す説明図、(b)は進行方向から見た説明図、第13図
(a)、(b)は従来の超電導磁気浮上方式鉄道用非接
触集電システムを示すもので、(a)は各種コイルの配
置を列車進行方向の横から見た状態を示す説明図、(b
)は車上の集電コイルによる集電状態を示す説明図、第
14図は集電コイルがコンバータ、バッファ用蓄電池お
よびインバータを介して負荷に接続された状態を示す説
明図である。 la、lb・・・浮上・推進用超電導コイル、3a。 3 b 、 3 c 、 3 d 、 3 e 、 3
 f−推進コイル、4 a + 4 b 94 c v
 4 d e 4 e * 4 f ・=浮上コイル、
6a、6b、6c、6d・・・集電用超電導コイル、7
a、7b、7c、7d、7e、7f−集電コイル、14
・・・昇降装置、15・・・クライオスタット(極低温
容器) 代理人 弁理士 高 橋 明 夫 (ほか1名) 第 図 区 第 図 第 図 15・・・タライオスタノト 第 図 第 図 第 図 第 図(a) 第 図fb)
Figures 1 (a) and (b) show the arrangement of a superconducting coil for current collection, a current collection coil, and a levitation coil in an embodiment of the non-contact current collection system for superconducting magnetic levitation railways of the present invention. )
is an explanatory diagram seen from the direction perpendicular to the traveling direction, (b) is an explanatory diagram seen from the same direction as the traveling direction, and FIG. 2 is another implementation of the superconducting magnetic levitation railway non-contact current collection system of the present invention. A superconducting coil for current collection viewed from a direction perpendicular to the traveling direction of the example.
An explanatory diagram showing the arrangement of current collecting coils and levitation coils, Figure 3 (
Figures a), (b), and (c) examine the effect of current collection according to Figures 1, 5, and 2, and (a) shows the required dimensions of the superconducting coil for current collection, the current collection coil, and the levitation coil, respectively. An explanatory diagram showing
(b) is an explanatory diagram showing the dimensions between the superconducting coil for current collection, the current collecting coil, and the levitation coil, (c) is an explanatory diagram showing the generated voltage, and Fig. 4 is a non-contact superconducting magnetic levitation system of the present invention for railways. A superconducting coil for levitation and propulsion in another embodiment of the current collection system, an explanatory diagram showing the pole pitch size of the superconducting coil for current collection, and FIGS. 5(a) and 5(b) show the superconducting magnetic levitation of the present invention. 6 shows the shape of the superconducting coil for current collection of still another embodiment of the non-contact current collection system for railways, (a) is a circular shape, (b) is an explanatory diagram when it is formed into an elliptical shape, The figure is an explanatory diagram showing the arrangement of the superconducting coil for current collection in still another embodiment of the superconducting magnetic levitation non-contact current collection system for railways of the present invention, and FIG. 7 shows that the superconducting coil for current collection has an adverse effect on the levitation characteristics. FIGS. 8(a) and 8(b) are explanatory diagrams showing the state in which the superconducting magnetic levitation type non-contact current collecting system for railways according to the present invention has a superconducting current collector that does not adversely affect the levitation characteristics of yet another embodiment of the non-contact current collecting system for railways. This shows the arrangement of the coil and current collector coil, (a
) is an explanatory diagram showing the case where the respective distances between these two coils are separated from the distance between the top and bottom of the levitation coil, and (b) is an explanatory diagram showing the case where the superconducting coil for current collection and the current collecting coil are provided with a lifting device. , FIG. 9 is an explanatory view showing a state in which the superconducting coil for current collection with a different polarity arrangement of still another embodiment of the superconducting magnetic levitation non-contact current collection system for railways of the present invention is stored in a cryostat. The figure is a waveform diagram of the three-phase sinusoidal current induced in the levitation coil by the current collecting superconducting coil.
Figures 11 (a) to (f) show the magnetic field distribution generated at the current collecting coil position by the sinusoidal current induced in the levitation coil, and (a) to (c) show the superconducting coil for current collecting. When the pole pitch of the superconducting coil for levitation and propulsion is 172, (a) is a composite wave, (b) is a fundamental wave, and (c) is a waveform diagram of a second spatial harmonic. (d) to (f) are cases in which the pole pitch of the superconducting coil for current collection is the same as the pole pitch of the superconducting coil for levitation and propulsion; (cl) is the composite wave, (e) is the fundamental wave, and (f) is the fifth wave. The waveform diagrams of the next spatial harmonics, Figure 12 (a) and (b), explain the basic movement of a conventional magnetic levitation train. (a) shows the arrangement of various coils from the side in the direction of train movement. 13(b) is an explanatory drawing showing the state as seen from the direction of travel, and FIGS. 13(a) and 13(b) show a conventional superconducting magnetic levitation type non-contact current collection system for railways. a) is an explanatory diagram showing the arrangement of various coils viewed from the side in the direction of train travel; (b)
) is an explanatory diagram showing a current collecting state by a current collecting coil on a vehicle, and FIG. 14 is an explanatory diagram showing a state in which the current collecting coil is connected to a load via a converter, a buffer storage battery, and an inverter. la, lb... superconducting coil for levitation and propulsion, 3a. 3 b, 3 c, 3 d, 3 e, 3
f-propulsion coil, 4 a + 4 b 94 c v
4 d e 4 e * 4 f ・=levitation coil,
6a, 6b, 6c, 6d... superconducting coil for current collection, 7
a, 7b, 7c, 7d, 7e, 7f - current collector coil, 14
...Elevating device, 15...Cryostat (cryogenic container) Agent: Patent attorney Akio Takahashi (and one other person) a) Figure fb)

Claims (1)

【特許請求の範囲】 1.地上に浮上コイル、推進コイルの地上コイル、車上
に浮上・推進用超電導コイルを備えたシステムの、前記
車上には車両の運動エネルギーを前記地上コイルを介し
て車両電力に変換する集電用超電導コイルおよび集電コ
イルが設けられている超電導磁気浮上方式鉄道用非接触
集電システムにおいて、前記集電用超電導コイルおよび
集電コイルが、前記浮上コイルのそれと同じようにその
上下に配置したコイル間を8の字状に接続してなる8字
形形状とされたものであることを特徴とする超電導磁気
浮上方式鉄道用非接触集電システム 2.前記集電用超電導コイルおよび集電コイルが、前記
浮上コイルのそれと同じようにその上下に配置したコイ
ル間を8の字状に接続してなる8字形形状に代えて、そ
の上下に配置したコイルが夫々異なる極を有している異
極配置とされたものである請求項1記載の超電導磁気浮
上方式鉄道用非接触集電システム 3.前記集電用超電導コイルが、同一の極低温容器に収
納されたものである請求項2記載の超電導磁気浮上方式
鉄道用非接触集電システム 4.前記集電用超電導コイルのポールピッチが、前記浮
上・推進用超電導コイルのポールピッチより小さくされ
たものである請求項1または請求項2記載の超電導磁気
浮上方式鉄道用非接触集電システム 5.前記集電用超電導コイルおよび集電コイルが、円形
状または楕円状に形成されたものである請求項1または
請求項2記載の超電導磁気浮上方式鉄道用非接触集電シ
ステム 6.前記集電用超電導コイルおよび集電コイルが、特定
の前記車両に搭載されるものである請求項1または請求
項2記載の超電導磁気浮上方式鉄道用非接触集電システ
ム 7.前記集電用超電導コイルおよび集電コイルが、その
上下に配置されたコイル間の距離を夫々前記浮上コイル
の上下間の距離よりも大きくされたものである請求項1
または請求項2記載の超電導磁気浮上方式鉄道用非接触
集電システム8.前記集電用超電導コイルおよび集電コ
イルが、昇降装置で上下に移動自在に形成されたもので
ある請求項1または請求項2記載の超電導磁気浮上方式
鉄道用非接触集電システム 9.地上に浮上コイル、推進コイルの地上コイル、車上
に浮上・推進用超電導コイルを備えたシステムの、前記
車上には車両の運動エネルギーを前記地上コイルを介し
て車両電力に変換する集電用超電導コイルおよび集電コ
イルが設けられている超電導磁気浮上方式鉄道用非接触
集電システムにおいて、前記集電用超電導コイルのポー
ルピッチが、前記浮上・推進用超電導コイルのポールピ
ッチより小さくされたものであることを特徴とする超電
導磁気浮上方式鉄道用非接触集電システム 10.地上に浮上コイル、推進コイルの地上コイル、車
上に浮上・推進用超電導コイルを備えたシステムの、前
記車上には車両の運動エネルギーを前記地上コイルを介
して車両電力に変換する集電用超電導コイルおよび集電
コイルが設けられている超電導磁気浮上方式鉄道用非接
触集電システムにおいて、前記集電用超電導コイルのポ
ールピッチが、前記浮上・推進用超電導コイルのポール
ピッチの1/2であることを特徴とする超電導磁気浮上
方式鉄道用非接触集電システム
[Claims] 1. In a system equipped with a levitation coil on the ground, a ground coil for propulsion coils, and a superconducting coil for levitation and propulsion on the vehicle, there is a current collector on the vehicle that converts the kinetic energy of the vehicle into vehicle power via the ground coil. In a non-contact current collection system for a superconducting magnetic levitation railway in which a superconducting coil and a current collecting coil are provided, the superconducting coil for current collecting and the current collecting coil are coils arranged above and below the levitation coil in the same manner as those of the levitation coil. 2. A superconducting magnetic levitation non-contact current collection system for railways, characterized in that it has a figure-8 shape in which the gaps are connected in a figure-8 shape. The superconducting coil for current collection and the current collecting coil are coils arranged above and below the levitation coil instead of having a figure 8 shape in which the coils arranged above and below are connected in a figure 8 shape. 3. A superconducting magnetic levitation type non-contact current collection system for railways according to claim 1, wherein the non-contact current collection system for railways according to claim 1 is arranged in a different pole arrangement, each having a different pole. 4. The superconducting magnetic levitation non-contact current collection system for railways according to claim 2, wherein the current collecting superconducting coils are housed in the same cryogenic container. 5. The superconducting magnetic levitation non-contact current collection system for railways according to claim 1 or 2, wherein the pole pitch of the current collection superconducting coil is smaller than the pole pitch of the levitation/propulsion superconducting coil. 6. The superconducting magnetic levitation non-contact current collecting system for railways according to claim 1 or 2, wherein the current collecting superconducting coil and the current collecting coil are formed in a circular or elliptical shape. 7. The superconducting magnetic levitation non-contact current collecting system for railways according to claim 1 or 2, wherein the current collecting superconducting coil and the current collecting coil are mounted on a specific vehicle. Claim 1: The current collecting superconducting coil and the current collecting coil each have a distance between the coils disposed above and below each other larger than a distance between the above and below the levitation coil.
or the superconducting magnetic levitation non-contact current collection system for railways according to claim 2;8. 9. The superconducting magnetically levitated non-contact current collecting system for railways according to claim 1 or 2, wherein the current collecting superconducting coil and the current collecting coil are formed to be movable up and down by a lifting device. In a system equipped with a levitation coil on the ground, a ground coil for propulsion coils, and a superconducting coil for levitation and propulsion on the vehicle, there is a current collector on the vehicle that converts the kinetic energy of the vehicle into vehicle power via the ground coil. A non-contact current collection system for a superconducting magnetic levitation railway that is provided with a superconducting coil and a current collecting coil, wherein the pole pitch of the current collecting superconducting coil is smaller than the pole pitch of the levitation/propulsion superconducting coil. 10. A superconducting magnetic levitation non-contact current collection system for railways characterized by: In a system equipped with a levitation coil on the ground, a ground coil for propulsion coils, and a superconducting coil for levitation and propulsion on the vehicle, there is a current collector on the vehicle that converts the kinetic energy of the vehicle into vehicle power via the ground coil. In a superconducting magnetic levitation non-contact current collection system for railways in which a superconducting coil and a current collecting coil are provided, the pole pitch of the current collecting superconducting coil is 1/2 of the pole pitch of the levitation/propulsion superconducting coil. A superconducting magnetic levitation railway non-contact current collection system characterized by
JP2124813A 1990-05-15 1990-05-15 Superconducting magnetic levitation non-contact current collection system for railways Expired - Fee Related JP2565582B2 (en)

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JP2124813A JP2565582B2 (en) 1990-05-15 1990-05-15 Superconducting magnetic levitation non-contact current collection system for railways

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Application Number Priority Date Filing Date Title
JP2124813A JP2565582B2 (en) 1990-05-15 1990-05-15 Superconducting magnetic levitation non-contact current collection system for railways

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JPH0421301A true JPH0421301A (en) 1992-01-24
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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0426302A (en) * 1990-05-16 1992-01-29 Central Japan Railway Co Current collector for magnetic levitation train
CN110752677A (en) * 2019-11-06 2020-02-04 北京交通大学 Vehicle-mounted linear generator for high-speed magnetic suspension train
CN113708508A (en) * 2020-05-21 2021-11-26 中国航天科工飞航技术研究院(中国航天海鹰机电技术研究院) Non-contact power supply device suitable for full-speed domain operation of maglev train
CN113696744A (en) * 2020-05-21 2021-11-26 中国航天科工飞航技术研究院(中国航天海鹰机电技术研究院) Vehicle-mounted wireless power transmission device suitable for vacuum pipeline maglev train

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5663550A (en) * 1979-10-31 1981-05-30 Fuji Electric Co Ltd Damping device for magnetic floating car
JPH01298902A (en) * 1988-05-27 1989-12-01 Railway Technical Res Inst Levitating, guiding and driving device for guided repulsion magnetic levitation railway

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5663550A (en) * 1979-10-31 1981-05-30 Fuji Electric Co Ltd Damping device for magnetic floating car
JPH01298902A (en) * 1988-05-27 1989-12-01 Railway Technical Res Inst Levitating, guiding and driving device for guided repulsion magnetic levitation railway

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0426302A (en) * 1990-05-16 1992-01-29 Central Japan Railway Co Current collector for magnetic levitation train
CN110752677A (en) * 2019-11-06 2020-02-04 北京交通大学 Vehicle-mounted linear generator for high-speed magnetic suspension train
CN113708508A (en) * 2020-05-21 2021-11-26 中国航天科工飞航技术研究院(中国航天海鹰机电技术研究院) Non-contact power supply device suitable for full-speed domain operation of maglev train
CN113696744A (en) * 2020-05-21 2021-11-26 中国航天科工飞航技术研究院(中国航天海鹰机电技术研究院) Vehicle-mounted wireless power transmission device suitable for vacuum pipeline maglev train
CN113696744B (en) * 2020-05-21 2023-08-15 中国航天科工飞航技术研究院(中国航天海鹰机电技术研究院) Vehicle-mounted wireless power transmission device suitable for vacuum pipeline maglev train

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