JPH01144357A - Superconducting coil quick cool motor - Google Patents

Superconducting coil quick cool motor

Info

Publication number
JPH01144357A
JPH01144357A JP62299288A JP29928887A JPH01144357A JP H01144357 A JPH01144357 A JP H01144357A JP 62299288 A JP62299288 A JP 62299288A JP 29928887 A JP29928887 A JP 29928887A JP H01144357 A JPH01144357 A JP H01144357A
Authority
JP
Japan
Prior art keywords
coil
current
permanent magnet
superconducting
temperature
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
JP62299288A
Other languages
Japanese (ja)
Inventor
Shinichi Watanabe
伸一 渡邊
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.)
Individual
Original Assignee
Individual
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 Individual filed Critical Individual
Priority to JP62299288A priority Critical patent/JPH01144357A/en
Publication of JPH01144357A publication Critical patent/JPH01144357A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain a turning effect of large quantity and large output by using a superconducting coil mounting a quick responsive cool device. CONSTITUTION:A permanent magnet 2 is arranged in a rotary shaft 4 in the center in a manner wherein polarity is obtained as shown in the drawing. While a superconducting coil (S coil) 1 is arranged in such a manner as to receive magnetic force of the permanent magnet. And leaving this S coil 1 in a condition of no flow of current further with normal conduction, the magnet is approached this coil 1, generating an electric current by electromagnetic induction. The moment the current of maximum quantity is allowed to flow in this coil 1, it is placed in a superconducting condition by a quick responsive cool device. As the result, continuing a flow as the permanent current in the S coil 1, it performs action similar to a permanent magnet.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、超電導コイルを制御利用し、回転力を得られ
るようにしたものである。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention utilizes and controls superconducting coils to obtain rotational force.

従来の技術 従来、モーターを回転させるためには電気を必要とし、
常に電気を流しておかねばならなかった。
Conventional technology Traditionally, electricity was required to rotate a motor.
Electricity had to be kept flowing at all times.

そのため大量の電気を常に消費しなければならなかった
Therefore, large amounts of electricity had to be constantly consumed.

問題を解決する手段 本発明は、その欠点を除くために発明されたものであり
図面第1図のように構成される。中心の回転軸に、永久
磁石が図のような極になるように配置してある。その磁
力を、受けるように超電導コイルが配置されているので
ある。回転原理の説明の前に、本発明が使用する、急速
反応冷温装置をとりつけた超電導コイル(以下Sコイル
とする)の作用を説明する。
Means for Solving the Problem The present invention was invented in order to eliminate this drawback, and is constructed as shown in FIG. 1 of the drawings. Permanent magnets are arranged around the central rotating shaft so that they form poles as shown in the figure. A superconducting coil is placed to receive the magnetic force. Before explaining the rotation principle, the operation of the superconducting coil (hereinafter referred to as S coil) equipped with a rapid reaction cooling device used in the present invention will be explained.

このSコイルを電流がいっさい流れていない状態にして
おき、又Sコイルの冷温環境の温度は、そのSコイルが
、超電導になる温度すなわち臨界温度に達していない状
態にしておく。Sコイルはまだ超電導状態の作用は表わ
れておらず、電流を流していない常電導コイルと同じで
ある。そのような状態のSコイルに磁石を、近づけて電
磁誘導により、電流を発生させ、その電流がSコイルに
最大量流れた瞬間に、急速反応冷温装置により、Sコイ
ルを急速冷却し瞬時に超電導状態にしてやる。そうする
事により、さきにSコイルに誘起された電流が瞬時のう
ちに、Sコイル自体が超電導状態になってしまうため永
久電流としてSコイルに流れ続ける事になるのである。
This S coil is kept in a state where no current flows, and the temperature of the cold environment of the S coil is kept so that the temperature at which the S coil becomes superconducting, that is, does not reach the critical temperature. The S coil has not yet exhibited the effects of a superconducting state, and is the same as a normal conducting coil in which no current is flowing. A magnet is brought close to the S coil in such a state and a current is generated by electromagnetic induction.At the moment when the maximum amount of current flows through the S coil, the S coil is rapidly cooled by a rapid reaction cooling device and instantaneously becomes superconducting. I'll make it into a state. By doing so, the current that was previously induced in the S coil instantaneously becomes a superconducting state, so that it continues to flow through the S coil as a persistent current.

そうすると、超電導コイルに電流を流すとその電流が永
久電流として流れつづけ、超電導コイルは永久磁石と同
じ作用をするため、Sコイルは永久磁石と同じようにな
ってしまうわけである。Sコイルに電流を発受させるた
め磁石を近づける状態の時はSコイルは超電導状態では
ないためマイナス効果は表われておらず、Sコイル内部
に磁力は入りこめるため発生する電流は、常電導のコイ
ルに、磁石を近づけて発生する電流とは、なんらかわり はない。電流を流したままで超電導状態にすると言う事
は、ある超電導材料の臨界温度を調べるなどと言う実験
方法と同じ事であり、すでに実証、証明されている。そ
れにより、Sコイルに誘起された電流は、永久電流とな
り保持されそのためSコイルは、永久磁石と同じような
作用をする事は、確かである。Sコイルに保持できる誘
起電流の量は、あらゆる技術的な面により大きくする事
が可能である。このような急速反応冷温装置を取りつけ
た超電導コイルの作用を利用して回転力を得るわけだ。
In this case, when a current is passed through a superconducting coil, the current continues to flow as a permanent current, and the superconducting coil acts in the same way as a permanent magnet, so the S coil becomes the same as a permanent magnet. When a magnet is brought close to the S coil in order to send and receive current, the S coil is not in a superconducting state, so no negative effect appears; the magnetic force can enter inside the S coil, so the generated current is normally conductive. This is no different from the current generated when a magnet is brought close to a coil. Developing a superconducting state while keeping current flowing is the same experimental method as investigating the critical temperature of a certain superconducting material, and it has already been demonstrated and proven. As a result, the current induced in the S coil becomes a permanent current and is maintained, so it is certain that the S coil acts in the same way as a permanent magnet. The amount of induced current that can be maintained in the S coil can be increased depending on various technical aspects. Rotational force is obtained by utilizing the action of a superconducting coil equipped with such a rapid reaction cooling device.

次に、図面第2,3図を見ていただきたい。これは、回
転原理を説明するために第1図を縮少、省略した部分断
面図であり、これにより回転原理を説明する。NOA,
B,Cとは自転軸につけられた永久磁石の番号であり、
NO1〜5とはSコイルにつけられた番号である。又、
矢印は回転方向を示しておりこの図では、図の矢印方向
に回転するように説明するが、実際は逆向きでもよい。
Next, I would like you to take a look at drawings 2 and 3. This is a partial cross-sectional view of FIG. 1 which is reduced and omitted in order to explain the principle of rotation, and the principle of rotation will be explained using this. NOA,
B and C are the numbers of permanent magnets attached to the rotation axis,
NO1-5 are numbers assigned to the S coils. or,
The arrow indicates the direction of rotation, and in this figure, it is explained that it rotates in the direction of the arrow in the figure, but in reality, it may be rotated in the opposite direction.

まず、第2図を見ていただきたい。First, please take a look at Figure 2.

SコイルNO1に、磁石NOAを、SコイルNO3に、
磁賎NOBを、SコイルNO5に磁石NOCをそれぞれ
近づける。もちろん電磁誘導により、電気を発生させる
わけだから、その近づける力は強ければ、強いほどいい
。そうすると、NO1,3,5のSコイルに、それぞれ
電磁誘導により電流が誘起される。その電流をSコイル
が瞬時に超電導状態になり永久電流として保持し、永久
磁石と同じ作用をするようになる。
S coil NO1, magnet NOA, S coil NO3,
Bring the magnet NOB closer to the S coil NO5 and the magnet NOC closer to the S coil NO5. Of course, electricity is generated by electromagnetic induction, so the stronger the force that brings it closer, the better. Then, currents are induced in the S coils of NO1, 3, and 5 by electromagnetic induction. The S coil instantaneously becomes superconducting and retains this current as a permanent current, causing it to function in the same way as a permanent magnet.

(この時の永久磁石とSコイルの位置関係は、Sコイル
の真上に、永久磁石が来ている状態になっている。つま
りSコイルの真上に永久磁石が来た瞬間に、Sコイルが
永久磁石による誘起電流を、永久電流として保持すると
考えられる。)すなわち、SBイルNO1は、S極、S
コイルNO3は、N極、SコイルNO5は、S極を、永
久磁石を近づけた例に発生するような、一種の永久“電
”磁石となるわけである。そうすると、NO1とNOA
、NO3とNOB、NO5とNOCの各Sコイルと永久
磁石は共に同極なので、当然反発し合う。その反発力は
矢印方向に、回転力を加えたため、矢印方向に反発し回
転する。
(The positional relationship between the permanent magnet and the S coil at this time is such that the permanent magnet is directly above the S coil.In other words, the moment the permanent magnet comes directly above the S coil, the S coil is considered to hold the induced current by the permanent magnet as a permanent current.) In other words, SB Illu NO1 has S pole, S
The coil NO3 is a north pole, and the S coil NO5 is a south pole, and they become a kind of permanent "electro" magnet, like the one that occurs when permanent magnets are brought close to each other. Then, NO1 and NOA
, NO3 and NOB, NO5 and NOC, and the permanent magnets have the same polarity, so naturally they repel each other. The repulsive force applies a rotational force in the direction of the arrow, so it rebounds and rotates in the direction of the arrow.

(ここまでの作用は、まだ回転加速段階と呼び、始動時
の状態にある。) そして、第3図のように回転軸が回り、今度はSコイル
NO2に、永久磁石NOB、SコイルNO4に永久磁石
NOCが、それぞれ近づく(近づかせる)。そうすると
前記の通りSコイルNO2がNOBの永久磁石によりN
極化し、SBイルNO4は、NOCの永久磁石によりS
極化するわけである。(この状態になってから、本回転
段階と呼び、本発明が自分自身で回転できる状態になる
(The action up to this point is still called the rotational acceleration stage, and is in the starting state.) Then, as shown in Figure 3, the rotating shaft rotates, and this time the S coil NO2, the permanent magnet NOB, and the S coil NO4 The permanent magnets NOC approach each other (make them approach each other). Then, as mentioned above, the S coil NO2 becomes N due to the NOB permanent magnet.
Polarized, SB illumination NO4 becomes S due to the permanent magnet of NOC.
It becomes polarized. (After this state is reached, it is called the main rotation stage, and the present invention is in a state where it can rotate by itself.

これにより、SコイルNO2と、永久磁石NOBは、同
極により、反発し合うと同時に、SコイルNO2のとな
りにあり、回転方向上にあるSコイルNO1は、永久磁
石NOAによりS極化しており永久磁石NOBとは異極
なので、引きつけ合い同時に発生する反発し合う力と引
きつけ合う力とで回転する。又SコイルNO4と、永久
磁石NOCは、同極により反発し合うと同時にSコイル
NO4のとなりにあり、回転方向上にあるSコイルNO
3は、永久磁石NOCと、異極のため引きつけ合うわけ
である。
As a result, the S coil NO2 and the permanent magnet NOB repel each other due to the same polarity, and at the same time, the S coil NO1, which is located next to the S coil NO2 and in the direction of rotation, is S-polarized by the permanent magnet NOA. Since it has a different polarity from the permanent magnet NOB, it rotates due to the attraction and repulsion forces that occur at the same time. Also, the S coil NO4 and the permanent magnet NOC repel each other due to the same polarity, and at the same time, the S coil NO4 is located next to the S coil NO4, and the permanent magnet NOC is located in the direction of rotation.
3 and the permanent magnet NOC are attracted to each other because they have different polarities.

しかし、そのままにしておいては、Sコイルと永久磁石
の異極同士が引きつけ合い最終的にSコイルの極が変わ
らないかぎり止まってしまう。
However, if left as is, the different polarities of the S coil and the permanent magnet will attract each other and eventually stop unless the S coil's polarity changes.

そこで、この図ではSコイルNO1と永久磁石NOB、
SコイルNO3と、永久磁石NOCとが引き合うわけだ
が、Sコイル(この図ではNO1,3)が永久磁石(こ
の図ではNOB,C)を引きよせ、ある程度(最適な位
置)まで引きつけたなら、SコイルNO1やNO3に流
れていた、永久電流をスイッチにより切り、Sコイルの
中から消しさると同時に、Sコイル(この図では、NO
1,NO3)自体を、超電導状態から常電導状態に、急
速反応冷温装置により、冷温環境の温度を上げて切りか
えてやる。それにより、Sコイル(この図では、NO1
,NO3)を、さきに永久磁石を近づける状態、すなわ
ち超電導状態になっておらず電流を流していない常電導
コイルと同じ状態にあるSコイルにもどしてやるのであ
る。
Therefore, in this figure, S coil NO1 and permanent magnet NOB,
S coil NO3 and permanent magnet NOC attract each other, but if the S coil (NO1, 3 in this figure) attracts the permanent magnet (NOB, C in this figure) to a certain degree (optimal position), The persistent current flowing through S coils NO1 and NO3 is turned off by a switch and is extinguished from inside the S coil. At the same time, the S coil (in this figure, NO
1, NO3) itself is switched from a superconducting state to a normal conducting state by raising the temperature of the cold environment using a rapid reaction cold temperature device. Thereby, the S coil (in this figure, NO1
, NO3) is returned to the S coil, which is in the same state as the normal conducting coil, which is not in the superconducting state and no current is flowing, which is the state in which the permanent magnet was brought close to it.

そうする事により、Sコイル(この図では、NO1,N
O3)に上記のように発生した、Sコイルと永久磁石と
の反発する力、引きつけ合う力により、永久磁石(この
国では、NOB,NOC)が近づき、電磁誘導により、
電流がそのSコイルに誘起され、その電流をSコイルに
永久電流として保持させるために、急速反応冷温装置に
より、Sコイルを、瞬時に、超電導状態にしてやる。そ
れにより、Sコイルが永久磁石と同じ作用をして近づい
た永久磁石(Sコイルに電流を誘起した永久磁石)と、
反発すると同時に、近づいた永久磁石のとなりにある永
久磁石を引きつけ回転軸を連続的に回転させるわけであ
る。
By doing so, the S coil (in this figure, NO1, N
O3) Due to the repulsive and attractive forces between the S coil and the permanent magnet, which occur as described above, the permanent magnets (NOB and NOC in this country) approach each other, and due to electromagnetic induction,
A current is induced in the S coil, and in order to maintain the current in the S coil as a permanent current, the S coil is instantaneously brought into a superconducting state by a rapid reaction cooling device. As a result, the S coil acts in the same way as a permanent magnet, and the permanent magnet approaches (the permanent magnet that induced a current in the S coil).
At the same time as it repels, it attracts the permanent magnet next to the approaching permanent magnet, causing the rotating shaft to rotate continuously.

こうして反発する力と、引きつけ合う力と言う、2つの
力が、永久磁石とSコイルの間におこり、回転軸が回転
していくわけである。もちろん第2図には省略されてい
る部分も、第1図のように同じ構造になっているため、
上記のSコイルと永久磁石との作用が連続的におこり、
本発明は回転するのである。
In this way, two forces, one of repulsion and the other of attraction, occur between the permanent magnet and the S coil, causing the rotating shaft to rotate. Of course, the parts omitted in Figure 2 have the same structure as in Figure 1, so
The action of the above S coil and permanent magnet occurs continuously,
The invention rotates.

本発明が回転するにあたって前記のように2つの段階に
わける事にする。1つは、回転加速段階で各Sコイルの
うち永久磁石により電流が、まだ誘起されていない(電
流が流れていない)物が、ある状態の事を言う2つめは
、本回転段階で各Sコイルすべてに永久磁石により、電
流が誘起された(電流が流れた)状態の事を言う。
The operation of the present invention is divided into two stages as described above. The first is that during the rotational acceleration stage, there is a state in which the current is not yet induced (current is not flowing) by the permanent magnet among the S coils. This refers to a state in which current is induced (current flows) in all coils by a permanent magnet.

本発明は、なんらかの方法で、本回転段階の状態までに
すれば、連続的に上記にような回転原理による作用がお
き、Sコイルを超電導状態に保ち制御してやれば、回転
するのである。しかし維ここで注意してもらいたい事が
ある。それは各Sコイルに、電流が流れているか、いな
いかにより、2つの段階にわかれるわけだが、その電流
とは、本発明の回転軸にとりつけている永久磁石により
電磁誘導によって発生した物を言い外部からの電流でな
いと言う事なのである。
In the present invention, if the state is brought to the main rotation stage by some method, the operation based on the rotation principle described above will occur continuously, and if the S coil is maintained in a superconducting state and controlled, it will rotate. However, there is something that I would like you to pay attention to here. It is divided into two stages depending on whether or not current is flowing through each S coil.The current is generated by electromagnetic induction from the permanent magnet attached to the rotating shaft of the present invention. This means that the current is not from.

本発明に使用される急速反応冷温装置とは、急速に反応
し、超電導コイルの冷温環境の温度を、ある温度に瞬間
的に、冷温して変化させるための装置と言う意味であり
固有名詞的な物ではなく、上記の作用をするのなら、た
とえ名称やその方法が違っていても、本発明の権利内に
ある。又、冷温と言う言葉の意味は、辞書(角川国語辞
典新版)などにより、つめたいことと、あたたかいこと
として、使っているわけだが、本発明の場合、日常言う
、つめたいとか、あたたかいなどと言うレベルではなく
、つめたいとは、Sコイルが母電導になる温度すなわち
臨界温度以下の事をさし、あたたかいとは、その臨界温
度よりも上の温度の事をさしている。このため、Sコイ
ルの臨界温度を“つめたい”とすると、誘起温度は“あ
たたかい”事として、意味をとるわけである。
The rapid reaction cold temperature device used in the present invention means a device that reacts rapidly and instantly changes the temperature of the cold environment of the superconducting coil to a certain temperature, and is a proper noun. Even if the name or method is different, if it performs the above-mentioned function, it is within the rights of the present invention. In addition, the meaning of the word ``cold temperature'' is used in dictionaries (Kadokawa Japanese Dictionary New Edition) as ``cold'' and ``warm,'' but in the case of the present invention, it is used at the level of everyday words such as ``cold'' and ``warm.'' Rather, "cold" refers to the temperature at which the S coil becomes conductive, that is, below the critical temperature, and "warm" refers to the temperature above that critical temperature. For this reason, if we say that the critical temperature of the S coil is "cold", the induced temperature is interpreted as "warm".

以上の冷温についての定番内での、非常に広い温度の事
を本発明での冷温と言う言葉は表わしている事を、理解
していただきたい。
Please understand that the term "cold temperature" in the present invention refers to a very wide range of temperatures within the above standard range of cold temperatures.

作用 このように、本発明は、なんらかの方法で本回転段階の
状態までにしてやれば、あとは、Sコイルを超電導状態
にし、上記の原理説明のような、制御を、してやれば外
部からの電力はもちろん、石油やガス、ウランなどの各
種燃料は、いっさい必要とせず、Sコイル冷温のための
冷温材料さえあれば連続的に回転するのである。又、冷
温材料は、一度使用したとしても又再液化などと言う形
で再利用でき限られた資源により、大量大出力の回転力
が得られるのである。
As described above, in the present invention, if the state of the main rotation stage is reached by some method, then the S coil is brought into a superconducting state and the control as explained above is performed, and then the power from the outside is reduced. Of course, there is no need for any kind of fuel such as oil, gas, or uranium; all you need is a cold material to keep the S coil cool and it will rotate continuously. Moreover, even if cold materials are used once, they can be reused by re-liquefaction, etc., and a large amount of high output torque can be obtained using limited resources.

しかし、本発明は、永久機関ではない。なぜなら本発明
は、なんらかのエネルギーを与えることなしに、動力を
増大させているわけではないからだ。どんなにしても、
Sコイルを超電導にするための冷却材(冷温材料)は、
絶対必要となる。すなわち完全には説明できないが、S
コイルを、超電導にするためのエネルギーが、本発明を
回転させる原動力となっているはずである。
However, the present invention is not a perpetual motion machine. This is because the present invention does not increase power without providing some kind of energy. No matter what,
The coolant (cold material) to make the S coil superconducting is
Absolutely necessary. In other words, although it cannot be fully explained, S
The energy required to make the coil superconducting should be the driving force that rotates the present invention.

現在まだ学理的、完全な説明はできないが、そのような
エネルギーを中心として、回転力に変えているはずであ
る。(この事は、永久磁石をエネルギー法則的に説明し
ようとする事とよくにている。) 本発明の回転原理の中核は、Sコイルが、永久磁石によ
る誘起電流を保持する事により、永久磁石と同じ作用を
すると言う現像であるわけだが、この現像は、前記の通
り、実証、証明されている。
Although it is not yet possible to provide a complete scientific explanation, it is believed that such energy is converted into rotational force. (This is similar to trying to explain permanent magnets in terms of the energy law.) The core of the rotation principle of the present invention is that the S coil maintains the induced current by the permanent magnet, This development is said to have the same effect as the above, and as mentioned above, this development has been proven and proven.

又、その保持する電流は、その電流が最大に表れた瞬間
に、超電導にするため減る事はないと考えられる。なぜ
なら、Sコイルに永久磁石により電流を誘起させる温度
すなわち誘起温度から臨界温度になる時間(以下、誘起
時間)が長ければ長いほど保持できる電流量は減ってい
く。しかし、本発明の場合、たとえ誘起時間はあるにし
ても、その時間を計算しSコイルに永久磁石が最大の電
流を誘起する時にちょうどSコイルが、超電導状態にな
るように急速反応冷温装置を、誘起時間分だけ前もって
作動させ、上記のように瞬時にSコイルに永久磁石が誘
起しうる最大電流を保持させる方法をとるわけだ。それ
にもし保持できる電流量が、常電導状態のSコイルの電
気抵抗により多少減るとしてもSコイルと永久磁石との
間に反発する力、引き合う力の2つが発生しているため
、それだけSコイルに永久磁が近づく速度は加速される
事になり、その分で多少減る分は補えるので常に一定値
を保持できる。このようにたとえ、まだエネルギー法則
の学理的面では、説明できないとは言え、本発明の原理
と、その効果は明確であり、特許法第29条にかかる発
明ではないと信ずる。
In addition, the current held by the superconductor is considered to be non-reduced at the moment when the current reaches its maximum level. This is because the longer the temperature at which a current is induced in the S coil by the permanent magnet, that is, the time from the induction temperature to the critical temperature (hereinafter referred to as induction time), the less the amount of current that can be maintained. However, in the case of the present invention, even if there is an induction time, the rapid reaction cooling device is used to calculate the induction time and set the S coil to a superconducting state just when the permanent magnet induces the maximum current in the S coil. , the S coil is activated in advance for the induction time, and the maximum current that can be induced by the permanent magnet is instantly maintained in the S coil as described above. Even if the amount of current that can be held is reduced somewhat due to the electrical resistance of the S coil in the normally conducting state, two forces, repulsive and attractive forces, are generated between the S coil and the permanent magnet, so the S coil The speed at which the permanent magnet approaches is accelerated, which compensates for the slight decrease, so it can always maintain a constant value. Even though this analogy cannot be explained in terms of the theory of energy law, the principle of the present invention and its effects are clear, and I believe that it is not an invention falling under Article 29 of the Patent Law.

実施例 本発明の実施態様には、個々に次のようなものがある。Example Individual embodiments of the invention include the following.

急速反応力温装置については、とにかく、Sコイルの冷
温環境の温度を急速瞬時に変えられる方法ならば、どん
な方法でもよいのだが1.冷温環境に、発熱材などを入
れこれにより温度をかえる方法 2.冷温環境自体を収縮、膨張、圧縮して、温度をかえ
る方法 3.冷温環境自体を出し入れする事により、温度をかえ
る方法 4.Sコイルの電流を調整して、Sコイル自体を発熱、
排熱する事により、温度をかえる方法5.前記の1,2
,3,4を、各種組み合わせて、温度をかえる方法 などが、考えられる。
Regarding the rapid reaction force temperature device, any method that can rapidly and instantaneously change the temperature of the cold environment of the S coil may be used.1. Method of changing the temperature by inserting a heat-generating material into a cold environment 2. A method of changing the temperature by contracting, expanding, and compressing the cold and hot environment itself 3. Method of changing the temperature by taking in and out the cold environment itself 4. By adjusting the current of the S coil, the S coil itself generates heat.
Method of changing temperature by exhausting heat 5. 1 and 2 above
, 3, and 4 may be combined in various ways to change the temperature.

本発明に使用する中心軸にとりつける磁石は、1.永久
磁石 2.超電導磁石などが考えられる。
The magnet attached to the central shaft used in the present invention is: 1. Permanent magnet 2. A superconducting magnet may be considered.

それから、本発明は、永久磁石と、Sコイルの数を多く
すればするほど回転力は、強くなるわけだが、そのため
に第1図には、永久磁石が4つ、Sコイルが8個しか、
書かれていないが、これを、もっと、ふやす方法、又第
1図の1つの構成を、タービン羽のように回転軸に、た
くさんつらねる方法もある。
In addition, in the present invention, the larger the number of permanent magnets and S coils, the stronger the rotational force becomes.
Although not mentioned, there is a way to increase this number even more, or to string many of the configurations shown in Figure 1 around the rotating shaft like turbine blades.

(上記に、冷温環境、冷温材料と言う言葉がでてきたが
、冷温環境とは、Sコイルを冷温するための環境条件の
事をさしており、冷温材料とは、Sコイルを冷温するた
めの、又冷温環境にするための材料、状態的な作用の事
をさしている。)発明の効果 本発明は、以上説明したような作用により、回転するわ
けだが、その回転力を利用して、発電する方法などと、
各種動力源として利用できる。しかも大出力が得られる
ので、大出力動力源とすれば、効果は、非常に大きくな
る。このように、実質的に、再利用できる、ある一定量
の限られた、冷温材料により、大量、大出力の回転力が
得られ産業におよぼす影響は、絶大であり、非常に画期
的である。
(The terms "cold environment" and "cold material" have been mentioned above, but the "cold environment" refers to the environmental conditions for cooling the S coil, and the "cold material" refers to the environmental conditions for cooling the S coil. (Also refers to the materials and state-related actions that create a cold environment.) Effects of the Invention The present invention rotates due to the actions described above, and uses the rotational force to generate electricity. how to do it, etc.
Can be used as a variety of power sources. Moreover, since a large output can be obtained, if it is used as a large output power source, the effect will be very large. In this way, a large amount of high-output rotational force can be obtained using a limited amount of reusable cold material, and the impact on industry is enormous and extremely groundbreaking. be.

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

第1図は、本発明の基本構成の断面図である。 第2,3図は、本発明の説明のため特別に、第1図の断
面図を、一部拡大した、部分断面図である。 1…超電導コイル 2…永久磁石 3…急速反応冷温装置 4…回転軸 5…モーター内部
FIG. 1 is a sectional view of the basic configuration of the present invention. 2 and 3 are partially enlarged sectional views of the sectional view of FIG. 1, especially for explaining the present invention. 1...Superconducting coil 2...Permanent magnet 3...Rapid reaction cooling device 4...Rotating shaft 5...Inside the motor

Claims (1)

【特許請求の範囲】[Claims]  超電導コイルを冷温するための冷温環境の温度を、急
速に変化させるための急速反応冷温装置をとりつけた超
電動コイルを、磁石と構成、配置しとことを、特徴とす
るモーター。
A motor characterized in that a superelectric coil equipped with a rapid reaction cooling device for rapidly changing the temperature of a cold environment for cooling a superconducting coil is configured and arranged with a magnet.
JP62299288A 1987-11-27 1987-11-27 Superconducting coil quick cool motor Pending JPH01144357A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62299288A JPH01144357A (en) 1987-11-27 1987-11-27 Superconducting coil quick cool motor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62299288A JPH01144357A (en) 1987-11-27 1987-11-27 Superconducting coil quick cool motor

Publications (1)

Publication Number Publication Date
JPH01144357A true JPH01144357A (en) 1989-06-06

Family

ID=17870592

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62299288A Pending JPH01144357A (en) 1987-11-27 1987-11-27 Superconducting coil quick cool motor

Country Status (1)

Country Link
JP (1) JPH01144357A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9637288B2 (en) 2011-12-21 2017-05-02 Nestec S.A. Sealable element for sealing a rim of receptacles

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US9637288B2 (en) 2011-12-21 2017-05-02 Nestec S.A. Sealable element for sealing a rim of receptacles

Similar Documents

Publication Publication Date Title
US5917261A (en) Motive power generating apparatus utilizing energy of permanent magnet
US6828890B2 (en) High intensity radial field magnetic array and actuator
US20050029819A1 (en) Bi-stable magnetic latch
JPH01144357A (en) Superconducting coil quick cool motor
ATE370636T1 (en) HEAT GENERATOR FOR MOTOR VEHICLES
Ohji et al. Permanent magnet bearings for horizontal-and vertical-shaft machines: A comparative study
CN110848104B (en) Mechanical iris device driven by shape memory alloy wire
WO2017158710A1 (en) Flywheel apparatus and power generation and driving motor apparatus
US20150061419A1 (en) Electric heating device with output greater than input
Vigneshwar et al. Comparison of radial flux PMSM and axial flux PMSM for hybrid electric tracked vehicles
JPH02159963A (en) Superconducting coil temperature conversion and control generation rotary machine
JP7064728B2 (en) Flywheel device and rotary electric machine
JPH02280694A (en) Actuator control circuit
CN208285177U (en) A kind of adjustable side set double salient-pole electric machine of suspending power
US7652549B2 (en) Bi-stable magnetic latch with permanent magnet stator
RU2310265C2 (en) Magnetic motor
Yi et al. Micro flywheel energy storage system with axial flux machine
JPH10303019A (en) Self-hold type rotary solenoid
GR1010357B (en) Straight drive motor-generator for free energy generation
McDonald Macroscopic Magnetic Forces Can Do Work
Karimov et al. Motor selection for aircraft active clearance control system
JP2003092870A (en) Motor
JP2002013468A (en) Static magnetic field type inertia prime mover
Liu et al. Optimal design of a micro axial flux switched-reluctance motor
JP3616856B2 (en) Bearing device

Legal Events

Date Code Title Description
RD05 Notification of revocation of power of attorney

Effective date: 20041209

Free format text: JAPANESE INTERMEDIATE CODE: A7425

A072 Dismissal of procedure

Free format text: JAPANESE INTERMEDIATE CODE: A072

Effective date: 20050329

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20080425

Year of fee payment: 5

FPAY Renewal fee payment (prs date is renewal date of database)

Year of fee payment: 6

Free format text: PAYMENT UNTIL: 20090425

FPAY Renewal fee payment (prs date is renewal date of database)

Free format text: PAYMENT UNTIL: 20100425

Year of fee payment: 7

LAPS Cancellation because of no payment of annual fees