JPS649672A - Superconducting magnetic element - Google Patents
Superconducting magnetic elementInfo
- Publication number
- JPS649672A JPS649672A JP62164533A JP16453387A JPS649672A JP S649672 A JPS649672 A JP S649672A JP 62164533 A JP62164533 A JP 62164533A JP 16453387 A JP16453387 A JP 16453387A JP S649672 A JPS649672 A JP S649672A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic path
- magnetic
- pole
- superconducting
- path
- 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
Landscapes
- Containers, Films, And Cooling For Superconductive Devices (AREA)
- Logic Circuits (AREA)
- Electronic Switches (AREA)
- Compositions Of Oxide Ceramics (AREA)
- Inorganic Compounds Of Heavy Metals (AREA)
Abstract
PURPOSE:To obtain a superconducting magnetic element having a functional property that a superconductive material shows a Meissner effect in a superconducting state and shows a ferromagnetism in a normal conducting state by a method wherein at least parts of magnetic paths are each composed of the superconductive material to show the ferrormagnetism at a superconducting critical temperature or higher. CONSTITUTION:A yoke 11 is connected to the N-pole and the S-pole of a permanent magnet 10. The point of the yoke 11 is divided into 2, a first magnetic path 12 and a second magnetic path 13 are constituted and a first superconductor magnetic path 120 and a second superconductor magnetic path 130, which are both constituted of a superconductive material, are each connected between the N-pole and the magnetic path 12, which is connected to the N-pole, and between the S-pole and the magnetic path 13, which is connected to the S-pole. When a control magnetic flux 20, which has an intensity equal almost with that of a magnetic flux 17 of the magnetic path 12 and has a reverse polarity, is applied to the magnetic path 12, the magnetic field in the magnetic path 12 is offset, is weakened and the magnetic path 120 is brought in a superconducting state. If the magnetic path 120 is brought in the superconducting state, the magnetic flux 17 flowing through the magnetic path 12 is turned to the magnetic path 13 and at the same time, superposes on the applied magnetic flux 20 to strengthen the intensities thereof each other. As a result, the superconducting state is collapsed to become a normal conductive state and a ferromagnetism is shown.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62164533A JPS649672A (en) | 1987-07-01 | 1987-07-01 | Superconducting magnetic element |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP62164533A JPS649672A (en) | 1987-07-01 | 1987-07-01 | Superconducting magnetic element |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPS649672A true JPS649672A (en) | 1989-01-12 |
Family
ID=15794969
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP62164533A Pending JPS649672A (en) | 1987-07-01 | 1987-07-01 | Superconducting magnetic element |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS649672A (en) |
-
1987
- 1987-07-01 JP JP62164533A patent/JPS649672A/en active Pending
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