JPH01122378A - Prime mover - Google Patents
Prime moverInfo
- Publication number
- JPH01122378A JPH01122378A JP27764387A JP27764387A JPH01122378A JP H01122378 A JPH01122378 A JP H01122378A JP 27764387 A JP27764387 A JP 27764387A JP 27764387 A JP27764387 A JP 27764387A JP H01122378 A JPH01122378 A JP H01122378A
- Authority
- JP
- Japan
- Prior art keywords
- rotor
- superconductors
- superconductor
- transition temperature
- prime mover
- 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
Links
- 239000002887 superconductor Substances 0.000 claims abstract description 45
- 230000007704 transition Effects 0.000 claims abstract description 22
- 230000005291 magnetic effect Effects 0.000 claims abstract description 17
- 230000000694 effects Effects 0.000 abstract description 5
- 238000001816 cooling Methods 0.000 abstract description 4
- 238000010438 heat treatment Methods 0.000 abstract description 2
- 238000010586 diagram Methods 0.000 description 3
- 230000005292 diamagnetic effect Effects 0.000 description 2
- 239000003638 chemical reducing agent Substances 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000003247 decreasing effect Effects 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
Landscapes
- Superconductive Dynamoelectric Machines (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明は低回転で高トルクが必要とされる原動機に関す
るものである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a prime mover that requires high torque at low rotation speeds.
従来の技術
原動機としては電気を用いる直流モータ、交流モータ、
ガソリンエンジン、蒸気機関のようなピストンを用いる
もの、タービンを用いるもの等がある。これらの原動機
は高速が要求されるもの。Conventional technology motors include DC motors, AC motors, and AC motors that use electricity.
There are engines that use pistons, such as gasoline engines and steam engines, and engines that use turbines. These prime movers require high speed.
高トルクが要求されるもの、小型が要求されるもの等、
使用目的により種々のものが存在する。Items that require high torque, items that require small size, etc.
There are various types depending on the purpose of use.
発明が解決しようとする問題点
ところが、以上の原動機は熱を直接エネルギとして用い
、小型、高トルクのものはなかった。Problems to be Solved by the Invention However, the above-mentioned prime movers use heat directly as energy, and there have been no small-sized, high-torque ones.
本発明は上記問題点に鑑み、磁界を印加した超電導体を
冷却し、完全反磁性とすることから力を得、簡単な構成
で、小型、高トルクの原動機を提供することを目的とす
る。In view of the above problems, it is an object of the present invention to provide a compact, high-torque prime mover with a simple configuration, which obtains power by cooling a superconductor to which a magnetic field is applied and making it completely diamagnetic.
問題点を解決するための手段
この目的を達成するために、本発明の原動機は、円柱状
の中心を回転軸としたロータと、ロータの側面の表面に
、ロータの回転軸に対称となるよう複数個固定された超
電導体と、一部の超電導体に磁場を印加する磁石と、磁
石により磁場が印加された超電導体を転移温度Tc以下
へ冷却する冷熱源と、その他の一部の超電導体を転移温
度10以上へ熱する温熱源によ多構成されることを特徴
とする。Means for Solving the Problems In order to achieve this object, the prime mover of the present invention includes a rotor with a cylindrical center as the rotation axis, and a rotor with a rotor on the side surface of the rotor so as to be symmetrical with the rotation axis of the rotor. A plurality of fixed superconductors, a magnet that applies a magnetic field to some of the superconductors, a cold source that cools the superconductor to which the magnetic field is applied by the magnet to below the transition temperature Tc, and some other superconductors It is characterized by comprising a heat source that heats the temperature to a transition temperature of 10 or more.
作用
本発明による作用は、超電導体が転移温度Tc以下に冷
却された時、完全反磁性を示し、超電導体の内部の磁場
が常にゼロであシ、外部の磁場を打ち消す向きに磁化す
るという、いわゆるマイスナー効果を用い、磁石付近の
超電導体のみを転移温度以下とすることで、駆動力を得
ることで実現する。Effect The effect of the present invention is that when a superconductor is cooled below the transition temperature Tc, it exhibits complete diamagnetic properties, the magnetic field inside the superconductor is always zero, and the superconductor is magnetized in a direction that cancels out the external magnetic field. This is achieved by using the so-called Meissner effect to obtain driving force by lowering only the superconductor near the magnet to a temperature below the transition temperature.
すなわち、回転軸に対して対称に、超電導体を配し、一
部の超電導体に磁石により磁場を印加し、冷熱源により
転移温度T。以下へ冷却する。すると、磁場が印加され
、転移温度−Tc以下へ冷却された超電導体のみに、超
電導体に印加される磁場が小さくなる方向へ超電導体が
移動する向きへ方が発生し、この力により回転トルクが
発生し、ロータを回転させ、原動機として動作する。こ
の時発生するトルクは、静止時にも発生するため、低回
転で高トルクが得られる原動機となる。That is, superconductors are arranged symmetrically with respect to the rotation axis, a magnetic field is applied to some of the superconductors by a magnet, and the transition temperature T is reached by a cold source. Cool to below. Then, a magnetic field is applied to the superconductor, which has been cooled to below the transition temperature -Tc, so that the superconductor moves in the direction in which the magnetic field applied to the superconductor becomes smaller, and this force causes rotational torque to increase. occurs, causing the rotor to rotate and act as a prime mover. The torque generated at this time is also generated when the engine is stationary, so it becomes a prime mover that can obtain high torque at low rotation speeds.
実施例
以下、本発明の一実施例について図面を参照しながら説
明する。第1図で、1は中心を回転軸とする円柱状のロ
ータ、22L〜2dはロータ1の側面の表面に、ロータ
1の回転軸に対して対称となるよう固定されている超電
導体、3a、3bは超電導体22L〜2dへ磁場を印加
する磁石、4は超電導体2+L〜2dを転移温度10以
上へ加熱するための温熱源、5は超電導体2a〜2dを
転移温度以下へ冷却するだめの冷熱源である。図では略
したが、ロータ1の回転から動力を得るための機構、磁
石32L 、 3b 、温熱源4.冷熱源6を固定する
ための構造体が必要である。EXAMPLE Hereinafter, an example of the present invention will be described with reference to the drawings. In FIG. 1, 1 is a cylindrical rotor with its rotation axis at the center, 22L to 2d are superconductors fixed to the side surface of the rotor 1 so as to be symmetrical with respect to the rotation axis of the rotor 1, and 3a , 3b is a magnet that applies a magnetic field to the superconductors 22L to 2d, 4 is a heat source for heating the superconductors 2+L to 2d to a transition temperature of 10 or higher, and 5 is a heat source for cooling the superconductors 2a to 2d to below the transition temperature. It is a source of cooling and heat. Although not shown in the figure, a mechanism for obtaining power from the rotation of the rotor 1, magnets 32L, 3b, heat source 4. A structure for fixing the cold source 6 is required.
第2図を用い、本実施例の動作を説明する。第2図は超
電導体の温度と抵抗の関係を示した図で、転移温度Tc
以下では抵抗が0となり、完全反磁性を示す。今、温熱
源4の温度をT4.冷熱源6の温度をT2(T2<To
<T、 )とし、ロータ1が第1図の位置にある時の超
電導体2&の温度をT3.超電導体2bの温度をT4.
超電導体2Cの温度をT5゜超電導体2dの温度をT6
とする。超電導体2a〜2dの温度T5〜T4が第2図
に示すように、次の関係である時、
To<T5(T、 ・・・・
・・(1)T2<T5〈To・・・・・・(2)
To<T4. T6(T5 ・・・
・・・(3)転移温度Tc以下の温度になり、磁場が印
加されている超電導体2cのみに、磁場が小さくなる方
向へ力fが働き、ロータ1は左回転することになる。ロ
ータ1が回転していくと、超電導体2Cの温度T5は転
移温度Tcを越え、力がなくなるが、この時、超電導体
2dの温度T6が下が9、転移温度以下となる、この時
前述したように、力が働き、ロータ1の回転を堅持する
。超電導体2a〜2dの温度が転移温度Tc以下となる
位置が、磁場の対称線より、冷熱源5に近い領域大であ
れば、ロータ1の回転方向は一意的に定まる。この位置
がBの領域であっても、ロータ1の回転がBから人の方
向(左回転)であれば、超電導体2a〜2dの比熱によ
り、ロータ1の回転中は、転移温度T。The operation of this embodiment will be explained using FIG. 2. Figure 2 is a diagram showing the relationship between temperature and resistance of a superconductor, with transition temperature Tc
Below, the resistance becomes 0 and complete diamagnetism is exhibited. Now, set the temperature of heat source 4 to T4. The temperature of the cold heat source 6 is set to T2 (T2<To
<T, ), and the temperature of the superconductor 2& when the rotor 1 is in the position shown in FIG. 1 is T3. The temperature of the superconductor 2b is set to T4.
The temperature of superconductor 2C is T5° The temperature of superconductor 2d is T6
shall be. As shown in FIG. 2, when the temperatures T5 to T4 of the superconductors 2a to 2d have the following relationship, To<T5(T, . . .
...(1) T2<T5<To...(2) To<T4. T6 (T5...
(3) Force f acts in the direction of decreasing the magnetic field only on the superconductor 2c whose temperature is below the transition temperature Tc and to which the magnetic field is applied, causing the rotor 1 to rotate counterclockwise. As the rotor 1 rotates, the temperature T5 of the superconductor 2C exceeds the transition temperature Tc and the force disappears, but at this time, the temperature T6 of the superconductor 2d decreases to 9, which is below the transition temperature, as mentioned above. As shown, the force acts and keeps the rotor 1 rotating. If the position where the temperature of the superconductors 2a to 2d becomes equal to or lower than the transition temperature Tc is in a large area closer to the cold source 5 than the line of symmetry of the magnetic field, the rotation direction of the rotor 1 is uniquely determined. Even if this position is in the region B, if the rotor 1 is rotating in the direction from B to the person (rotation to the left), the specific heat of the superconductors 2a to 2d will keep the rotor 1 at a transition temperature T during the rotation.
以下となる位置が人の領域とな9、回転が持続するQ
第1図で、温熱源4と冷熱源5の働きを交換すれば、ロ
ータ1の回転方向は右回υとなる。また磁石3bを冷熱
源5に対し、反対の位置へ置いてもロータ1の回転方向
が逆になり、ロータ1の回転方向の制御が可能である。The following positions are in the human area9, and the rotation continues Q In Fig. 1, if the functions of the heat source 4 and the cold source 5 are exchanged, the rotation direction of the rotor 1 will be clockwise υ. Further, even if the magnet 3b is placed in a position opposite to the cold source 5, the rotational direction of the rotor 1 is reversed, and the rotational direction of the rotor 1 can be controlled.
また冷熱源5.温熱源4の温度2位置、磁石3a 、
3bの磁場の強さ、位置によりロータ1の回転速度の制
御が可能である。磁石3aは、熱源の交換を行わない場
合必要でない。Also a cold source 5. Temperature 2 position of heat source 4, magnet 3a,
The rotational speed of the rotor 1 can be controlled by the strength and position of the magnetic field 3b. The magnet 3a is not required if the heat source is not replaced.
また転移温度Tcが室温以下の場合、温熱源4が、転移
温度Tcが室温以上の場合、冷熱源5が必ずしも必要と
されない。Furthermore, when the transition temperature Tc is below room temperature, the heat source 4 is not necessarily required, and when the transition temperature Tc is above room temperature, the cold source 5 is not necessarily required.
なお、本実施例では超電導体は4つに分割しであるが、
第3図に示すように、ロータ1の表面。In this example, the superconductor is divided into four parts, but
As shown in FIG. 3, the surface of the rotor 1.
全体をおおうものであっても同様の動作をする。Even if it covers the whole thing, it works in the same way.
発明の効果
以上のように本発明の原動機は、超電導体が固定された
ロータと磁石、熱源という簡単な構成であり、熱から直
接駆動力を得ることができる。また低速度で高トルクを
発生することから、減速機等を必要とせず、簡単な構成
で動力を伝達することが可能となる。Effects of the Invention As described above, the prime mover of the present invention has a simple structure consisting of a rotor to which a superconductor is fixed, a magnet, and a heat source, and can obtain driving force directly from heat. Furthermore, since high torque is generated at low speeds, power can be transmitted with a simple configuration without the need for a speed reducer or the like.
第1図は本発明の一実施例における原動機の構成を示す
概略図、第2図は同原動機の温度と超電導体の抵抗の関
係を示す特性図、第3図は本発明の他の実施例の構成を
示す概略図である。
1・・・・・・ロータ、2,2&〜2d・・山・超電導
体、32L 、 3t)・・・・・・磁石、4・・・・
・・温熱源、5・旧・・冷熱源0
代理人の氏名 弁理士 中 尾 敏 男 はが1名7−
−−ロータ
20〜2d−一一月1L番林
3α、ab−磁石
4−一一温気源
5−一一冷\熱派
第1図
/
第2図
第3図Figure 1 is a schematic diagram showing the configuration of a prime mover in one embodiment of the present invention, Figure 2 is a characteristic diagram showing the relationship between the temperature of the prime mover and the resistance of the superconductor, and Figure 3 is another embodiment of the present invention. FIG. 1...Rotor, 2,2&~2d...Mountain/superconductor, 32L, 3t)...Magnet, 4...
・Heat source, 5 Old ・Cold source 0 Agent's name Patent attorney Toshi Nakao Male 1 person 7-
--Rotor 20~2d-November 1L Banbayashi 3α, ab-Magnet 4-11 Hot air source 5-11 Cold\hot fan Fig. 1/ Fig. 2 Fig. 3
Claims (4)
タの側面の表面に、前記ロータの回転軸に対称となるよ
う複数個固定された超電導体と、一部の前記超電導体に
磁場を印加する磁石と、前記磁石により磁場が印加され
た前記超電導体を転移温度T_c以下へ冷却する冷熱源
と、その他の一部の前記超電導体を転移温度T_c以上
に熱する温熱源を複数備えた原動機。(1) A rotor with a cylindrical center as its rotation axis, a plurality of superconductors fixed to the surface of the side surface of the rotor so as to be symmetrical to the rotation axis of the rotor, and a magnetic field applied to some of the superconductors. , a cold source that cools the superconductor to which a magnetic field is applied by the magnet to below the transition temperature T_c, and a plurality of hot sources that heat some of the superconductors above the transition temperature T_c. prime mover.
が可能であり、前記温熱源、前記冷熱源により熱される
あるいは冷却される超電導体に磁場を印加する磁石が、
前記温熱源からロータの回転軸を見た位置と、前記冷熱
源から前記ロータの回転軸を見た位置が対称となる位置
へ複数備えられたことを特徴とする特許請求の範囲第1
項記載の原動機。(2) The hot source and the cold source can exchange their positions, and the magnet that applies a magnetic field to the superconductor heated or cooled by the hot source and the cold source,
Claim 1: A plurality of rotors are provided at positions where the position from the heat source viewed from the rotation axis of the rotor and the position from the cold heat source viewed from the rotation axis of the rotor are symmetrical.
The prime mover described in section.
おおうことを特徴とする特許請求の範囲第1項記載の原
動機。(3) The prime mover according to claim 1, wherein the superconductor covers at least the entire surface of the side surface of the rotor.
ら供給されることを特徴とする特許請求の範囲第1項記
載の原動機。(4) The prime mover according to claim 1, wherein at least one of the heat source and the cold source is supplied from the outside.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27764387A JPH01122378A (en) | 1987-11-02 | 1987-11-02 | Prime mover |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP27764387A JPH01122378A (en) | 1987-11-02 | 1987-11-02 | Prime mover |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH01122378A true JPH01122378A (en) | 1989-05-15 |
Family
ID=17586287
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP27764387A Pending JPH01122378A (en) | 1987-11-02 | 1987-11-02 | Prime mover |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH01122378A (en) |
-
1987
- 1987-11-02 JP JP27764387A patent/JPH01122378A/en active Pending
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