JPS6423516A - Superconducting transformer - Google Patents
Superconducting transformerInfo
- Publication number
- JPS6423516A JPS6423516A JP62178952A JP17895287A JPS6423516A JP S6423516 A JPS6423516 A JP S6423516A JP 62178952 A JP62178952 A JP 62178952A JP 17895287 A JP17895287 A JP 17895287A JP S6423516 A JPS6423516 A JP S6423516A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- flux density
- winding
- low
- windings
- 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
Classifications
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Abstract
PURPOSE:To reduce a loss of a winding to the utmost and to obtain a low-coat and small-sized superconducting transformer by a method wherein a part with the high magnetic-flux density of the winding is composed of a normal and the remaining part is composed of a superconductor. CONSTITUTION:A low-voltage winding 2 and a high-voltage winding 3 are wound on an iron core 1 via an appropriate reactance gap 4. An outer circumference side 2' at the low- voltage winding 2 and an inner circumference side 3' at the high-voltage winding 3 are composed of a normal conductor; the other windings situated at opposite sides of the reactance gap are composed of an oxide superconductor. By this constitution, the magnetic flux inside the windings is distributed in such a way that the magnetic-flux density becomes a minimum at a part opposite to the reactance gap 4 of the windings and that the magnetic-flux density becomes a maximum at a part of the reactance gap. The part with the high magnetic-flux density is composed of a normal conductor winding; because the critical-current density is large at the part with the low magnetic-flux density, a cross-sectional area of the superconductor can be reduced. In addition, the whole windings are kept at a low temperature until the superconductor displays a superconducting phenomenon, the resistivity in the normal conductor is lowered in accordance with the temperature; if, e.g, a copper wire is used and an operation is executed at the temperature of liquid nitrogen, a loss is reduced.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62178952A JPS6423516A (en) | 1987-07-20 | 1987-07-20 | Superconducting transformer |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP62178952A JPS6423516A (en) | 1987-07-20 | 1987-07-20 | Superconducting transformer |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6423516A true JPS6423516A (en) | 1989-01-26 |
Family
ID=16057527
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP62178952A Pending JPS6423516A (en) | 1987-07-20 | 1987-07-20 | Superconducting transformer |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6423516A (en) |
-
1987
- 1987-07-20 JP JP62178952A patent/JPS6423516A/en active Pending
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