JPH01112712A - magnetic levitation device - Google Patents

magnetic levitation device

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Publication number
JPH01112712A
JPH01112712A JP62270667A JP27066787A JPH01112712A JP H01112712 A JPH01112712 A JP H01112712A JP 62270667 A JP62270667 A JP 62270667A JP 27066787 A JP27066787 A JP 27066787A JP H01112712 A JPH01112712 A JP H01112712A
Authority
JP
Japan
Prior art keywords
magnetic flux
levitation device
superconductor
magnetic
magnetic levitation
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.)
Pending
Application number
JP62270667A
Other languages
Japanese (ja)
Inventor
Hisaaki Gyoten
久朗 行天
Koji Gamo
孝治 蒲生
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.)
Panasonic Holdings Corp
Original Assignee
Matsushita Electric Industrial Co Ltd
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 Matsushita Electric Industrial Co Ltd filed Critical Matsushita Electric Industrial Co Ltd
Priority to JP62270667A priority Critical patent/JPH01112712A/en
Publication of JPH01112712A publication Critical patent/JPH01112712A/en
Pending legal-status Critical Current

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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 本発明による磁気浮上装置は、輸送運搬機器、と9わけ
室内用など小型運搬機器、及び磁気浮上スピーカーなど
の小型弱電機器に利用される。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The magnetic levitation device according to the present invention is used in transportation equipment, especially small-sized transportation equipment such as indoor equipment, and small-sized weak electrical equipment such as magnetically levitated speakers.

従来の技術 超伝導を利用した磁気浮上装置としては、超伝導コイル
の作る超強磁場を用いたものに対し、超伝導体が磁束の
侵入を許さないというマイスナー効果を用いた装置やそ
ねらを複合した装置が考えられている〔資源・エネルギ
ー面からの超伝導技術に関する調査(科学技術庁資源調
査新資料144号)〕。例えば第3図に示すように、F
e、Goなどの強磁性材料から成る永久磁石、もしくは
電磁石でできた磁束発生体と、板状超伝導体との間の反
発力を利用した磁気浮上装置である。
Conventional technology Magnetic levitation devices using superconductivity include devices that use the Meissner effect, in which the superconductor does not allow magnetic flux to penetrate, whereas those that use the ultra-strong magnetic field created by superconducting coils. A composite device is being considered [Survey on superconducting technology from the perspective of resources and energy (Science and Technology Agency Resource Survey New Material No. 144)]. For example, as shown in Figure 3, F
This is a magnetic levitation device that utilizes the repulsive force between a magnetic flux generator made of a permanent magnet or an electromagnet made of a ferromagnetic material such as e, Go, etc., and a plate-shaped superconductor.

この磁気浮上装置においては、磁束発生体から発生した
磁束が完全反磁性である超伝導体によって湾曲し、板状
超伝導体の下部で密度が高くなる。
In this magnetic levitation device, the magnetic flux generated from the magnetic flux generating body is curved by the completely diamagnetic superconductor, and the density becomes high below the plate-shaped superconductor.

磁場のエネルギーは磁束密度の二乗に比例するので、板
状超伝導体下部の磁束@度を小さくする方向、すなわち
上方向に力が作用する。したがって強い浮上刃を得よう
とすれば、板状超伝導体下部の磁束密度が板状超伝導体
の位置によって太きく変化する構造にする必要がある。
Since the energy of the magnetic field is proportional to the square of the magnetic flux density, a force acts in a direction that reduces the magnetic flux below the plate-shaped superconductor, that is, in an upward direction. Therefore, in order to obtain a strong floating blade, it is necessary to create a structure in which the magnetic flux density at the bottom of the plate-shaped superconductor varies greatly depending on the position of the plate-shaped superconductor.

発明が解決しようとする問題点 しかしながら、磁束発生装置として第3図に示しだよう
な通常の構成をとるならば、浮上している板状超伝導体
が磁束発生装置に極めて近づいた際、第4図に示すよう
に磁束は強磁性芯材内で湾曲することによって、板状超
伝導体下部で磁束密度が高くなることを避ける。その結
果、浮上刃はある一定の範囲内に抑えられ、大きくはな
らない。
Problems to be Solved by the Invention However, if the magnetic flux generator has a normal configuration as shown in FIG. As shown in Fig. 4, the magnetic flux is curved within the ferromagnetic core material to prevent the magnetic flux density from increasing at the bottom of the plate-shaped superconductor. As a result, the floating blade is kept within a certain range and does not become large.

問題点を解決するための手段 本発明は板状超伝導体が磁束発生装置に近づいた時、強
磁性芯材内部での磁束の湾曲を防ぐために、強frki
性芯材を好ましくは細線化し、それぞれを超伝導材料で
包み込んだ構成を手段として提供するものである。
Means for Solving the Problems The present invention provides a strong frki
The present invention provides a structure in which the core material is preferably made into thin wires and each wire is wrapped in a superconducting material.

作用 本発明の手段によれば、強磁性芯材内部の磁束は包まれ
た超伝導体中を通ることができないので、芯材内部での
湾曲は起こらず、開放された芯材端面から発生する。そ
の結果、浮上する板状超伝導体がこの開放芯材端面に近
づくにつれ、磁束密度は非常に大きくなる。実際は板状
超伝導体と磁束発生装置との間のわずかのすきまから磁
束が漏れるので磁束密度は発散しないが、板状超伝導体
に作用する力は発散的に大きくなる。
According to the means of the present invention, the magnetic flux inside the ferromagnetic core cannot pass through the wrapped superconductor, so no curvature occurs inside the core, but is generated from the open end face of the core. . As a result, as the floating plate-shaped superconductor approaches the end face of the open core material, the magnetic flux density becomes extremely large. In reality, magnetic flux leaks through a small gap between the plate-shaped superconductor and the magnetic flux generator, so the magnetic flux density does not diverge, but the force acting on the plate-shaped superconductor increases in a divergent manner.

実施例 本発明の実施例を第1図に示す。磁束発生装置としては
Fe系の永久磁石を芯材1とし、その外側?組成式YB
a2Cu30p−δ等の酸化物からなる超伝導材料2で
包んだ線材を複数本たばねて補強した。超伝導材料2の
厚さは1間で一定とし、芯材の径を0.1 cm 、 
1 cm 、 5cmと変えた構成とした。
EXAMPLE An example of the present invention is shown in FIG. As a magnetic flux generator, an Fe-based permanent magnet is used as the core material 1, and the outside? Composition formula YB
A plurality of wire rods wrapped in a superconducting material 2 made of an oxide such as a2Cu30p-δ were reinforced by folding them together. The thickness of the superconducting material 2 is constant at 1 cm, the diameter of the core material is 0.1 cm,
The configurations were changed to 1 cm and 5 cm.

板状超伝導体3としては厚さ2 MM、直径2cmの円
盤状の同じく組成式YBa2Cu309−,5の酸化物
超伝導体2の焼結物を用いた。
As the plate-shaped superconductor 3, a disk-shaped sintered product of the oxide superconductor 2 having the same compositional formula YBa2Cu309-,5 was used, having a thickness of 2 mm and a diameter of 2 cm.

液体窒素温度において、両者を2Hまで接近させた時に
かかる反発力を浮上刃として測定した。
At liquid nitrogen temperature, the repulsive force exerted when the two were brought close to each other up to 2H was measured as a floating blade.

その結果を、従来の方法すなわち超伝導材料で包まない
永久磁石を用いた時の浮上刃と比較して1表にあられし
た。
The results are shown in Table 1 in comparison with the conventional method, that is, when using a permanent magnet that is not wrapped in superconducting material.

(以下余 白) 本発明による方法は従来の方法と比較すると格段に強い
浮上刃を得ることができた。また芯材の径が5cmのも
のより、I Cm 、 I Mllと小さくなるにつれ
飛躍的に強い浮上刃が得られているが、芯材の径が板状
超伝導体に比べて小さい程、芯材端面から発生した磁束
を塞ぐ効果が大きいことを表している。したがってより
大きい浮上刃を得ようとすると、より小さい径の強磁性
芯材と、それを包む超伝導体で構成される線材を多数本
たばねて磁束発生端面を形成する方がよいことがわかっ
た。
(The following is a blank space) The method according to the present invention was able to obtain a floating blade that was much stronger than the conventional method. In addition, as the diameter of the core material becomes smaller to I Cm and I Mll, a dramatically stronger floating blade is obtained than when the diameter of the core material is 5 cm. This indicates that the effect of blocking the magnetic flux generated from the edge of the material is large. Therefore, in order to obtain a larger floating blade, it was found that it is better to form a magnetic flux-generating end surface by forming a large number of wires made of a ferromagnetic core material with a smaller diameter and a superconductor surrounding it. .

この実施例では、互いに反発する一方に磁束発生装置と
もう一方に板状超伝導体を用いたが、第2図に示すよう
に本発明による一対の磁束発生装置を用いても同様に強
い浮上刃が得られることは明らかである。また、本発明
による強力な浮上刃は、強磁性芯材を取り巻く超伝導材
料のマイスナー効果に由来するものであるので、例えば
常温でマイスナー効果を有する材料を用いて、磁束発生
装置を構成した時には常温で強力な浮上刃が得られるこ
とはいうまでもない。
In this example, a magnetic flux generator was used on one side and a plate-shaped superconductor was used on the other side, but as shown in Figure 2, even if a pair of magnetic flux generators according to the present invention is used, the same strong levitation can be obtained. It is clear that the blade is obtained. Furthermore, the strong floating blade of the present invention is derived from the Meissner effect of the superconducting material surrounding the ferromagnetic core material, so for example, when a magnetic flux generator is constructed using a material that has the Meissner effect at room temperature, Needless to say, a strong floating blade can be obtained at room temperature.

発明の効果 本発明のように、強磁性体と超伝導体の比較的単純な構
成によって強力な浮上刃が得られると、輸送・運搬技術
に与える効果は計り知れない。
Effects of the Invention If a strong floating blade can be obtained with a relatively simple structure of ferromagnetic material and superconductor as in the present invention, the effect on transportation and transportation technology will be immeasurable.

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

第1図は強磁性芯材を超伝導体で包んだ構成の本発明の
一実施例の磁気浮上装置における磁束分布図、第2図は
一対の磁束発生装置からなる本発明の異なる実施例の磁
気浮上装置における磁束分布図、第3図および第4図は
従来例の磁気浮上装置において、板状超伝導体がそれぞ
れ離れている時と近接した時の磁束分布図である。 1・・・・・・強磁性芯材、2・・・・・・超伝導体、
3・・・・・・板状超伝導体。 代理人の氏名 弁理士 中 尾 敏 男 はが1名第1
図 第2図
Fig. 1 is a magnetic flux distribution diagram in a magnetic levitation device according to an embodiment of the present invention in which a ferromagnetic core material is wrapped with a superconductor, and Fig. 2 is a diagram of a magnetic flux distribution in a different embodiment of the present invention consisting of a pair of magnetic flux generating devices. Magnetic flux distribution diagrams in a magnetic levitation device. FIGS. 3 and 4 are magnetic flux distribution diagrams when plate-shaped superconductors are separated and close to each other, respectively, in a conventional magnetic levitation device. 1...Ferromagnetic core material, 2...Superconductor,
3...Plate superconductor. Name of agent: Patent attorney Toshio Nakao (1st person)
Figure 2

Claims (3)

【特許請求の範囲】[Claims] (1)少なくとも一方の磁束発生装置が強磁性芯材とそ
れを包む超伝導材料によって構成されることを特徴とす
る磁気浮上装置。
(1) A magnetic levitation device characterized in that at least one magnetic flux generating device is composed of a ferromagnetic core material and a superconducting material surrounding it.
(2)強磁性芯材の開放された磁束発生端面が、対置す
る浮上装置の超伝導材料面よりも小さいことを特徴とす
る特許請求の範囲第1項記載の磁気浮上装置。
(2) The magnetic levitation device according to claim 1, wherein the open magnetic flux generating end surface of the ferromagnetic core material is smaller than the superconducting material surface of the opposing levitation device.
(3)超伝導材料として酸化物超伝導体を用いる特許請
求の範囲第1項または第2項記載の磁気浮上装置。
(3) A magnetic levitation device according to claim 1 or 2, in which an oxide superconductor is used as the superconducting material.
JP62270667A 1987-10-27 1987-10-27 magnetic levitation device Pending JPH01112712A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62270667A JPH01112712A (en) 1987-10-27 1987-10-27 magnetic levitation device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62270667A JPH01112712A (en) 1987-10-27 1987-10-27 magnetic levitation device

Publications (1)

Publication Number Publication Date
JPH01112712A true JPH01112712A (en) 1989-05-01

Family

ID=17489269

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62270667A Pending JPH01112712A (en) 1987-10-27 1987-10-27 magnetic levitation device

Country Status (1)

Country Link
JP (1) JPH01112712A (en)

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