Frozen mirror image method

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Fig. 1. Illustration of the frozen mirror image method for a simplest case of the magnetic dipole over the flat superconducting surface. Frozen image method.png
Fig. 1. Illustration of the frozen mirror image method for a simplest case of the magnetic dipole over the flat superconducting surface.

Frozen mirror image method (or method of frozen images) is an extension of the method of images for magnet-superconductor systems that has been introduced by Alexander Kordyuk in 1998 to take into account the magnetic flux pinning phenomenon. [1] The method gives a simple representation of the magnetic field distribution generated by a magnet (a system of magnets) outside an infinitely flat surface of a perfectly hard (with infinite pinning force) type-II superconductor in more general field cooled (FC) case, i.e. when the superconductor goes into superconducting state been already exposed to the magnetic field. The difference from the mirror image method, which deals with a perfect type-I superconductor (that completely expels the magnetic field, see the Meissner effect), is that the perfectly hard superconductor screens the variation of the external magnetic field rather than the field itself.

Contents

Description

The name originates from the replacement of certain elements in the original layout with imaginary magnets, which replicates the boundary conditions of the problem (see Dirichlet boundary conditions). In a simplest case of the magnetic dipole over the flat superconducting surface (see Fig. 1), the magnetic field, generated by a dipole moved from its initial position (at which the superconductor is cooled to the superconducting state) to a final position and by the screening currents at the superconducting surface, is equivalent to the field of three magnetic dipoles: the real one (1), its mirror image (3), and the mirror image of it in initial (FC) position but with the magnetization vector inversed (2).

Applications

The method is shown to work for the bulk high temperature superconductors (HTSC), [1] which are characterized by strong pinning and used for calculation of the interaction in magnet-HTSC systems such as superconducting magnetic bearings, [2] superconducting flywheels, [3] MAGLEV, [2] [4] for spacecraft applications, [5] [6] as well as a textbook model for science education. [7]

See also

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Flux pinning

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Halbach array

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Flywheel energy storage

Flywheel energy storage (FES) works by accelerating a rotor (flywheel) to a very high speed and maintaining the energy in the system as rotational energy. When energy is extracted from the system, the flywheel's rotational speed is reduced as a consequence of the principle of conservation of energy; adding energy to the system correspondingly results in an increase in the speed of the flywheel.

Magnetic levitation the method by which an object is suspended with no support other than magnetic fields

Magnetic levitation (maglev) or magnetic suspension is a method by which an object is suspended with no support other than magnetic fields. Magnetic force is used to counteract the effects of the gravitational acceleration and any other accelerations.

Alexander A. Kordyuk is a Ukrainian experimental physicist, known mainly for invention of the Method of frozen images and several experimental techniques based on magnetic levitation, and for contribution to the field of high temperature superconductivity.

References

  1. 1 2 Kordyuk, A. A. (1998). "Magnetic levitation for hard superconductors" (PDF). Journal of Applied Physics . 83 (1): 610–611. Bibcode:1998JAP....83..610K. doi:10.1063/1.366648.
  2. 1 2 Hull, John R. (2000). "Superconducting bearings". Superconductor Science and Technology . 13 (2): R1–R15. Bibcode:2000SuScT..13R...1H. doi:10.1088/0953-2048/13/2/201. ISSN   1361-6668.
  3. Filatov, A. V.; Maslen, E. H. (November 2001). "Passive magnetic bearing for flywheel energy storage systems". IEEE Transactions on Magnetics . 37 (6): 3913–3924. Bibcode:2001ITM....37.3913F. doi:10.1109/20.966127.
  4. Liu, W.; Wang, J. S.; Jing, H.; Jiang, M.; Zheng, J.; Wang, S. Y. (2008). "Levitation performance of high-Tc superconductor in sinusoidal guideway magnetic field". Physica C: Superconductivity . 468 (23): 2345–2350. Bibcode:2008PhyC..468.2345L. doi:10.1016/j.physc.2008.08.011.
  5. Shoer, J. P.; Peck, M. A. (2009). "Flux-pinned interfaces for the assembly, manipulation, and reconfiguration of modular space systems" (PDF). Journal of the Astronautical Sciences. 57 (3): 667. Bibcode:2009JAnSc..57..667S. doi:10.1007/BF03321521. S2CID   16573560. Archived from the original (PDF) on 2011-11-03.
  6. Norman, M. C.; Peck, M. A. (2010). "Stationkeeping of a flux-pinned satellite network" (PDF). Journal of Guidance, Control, and Dynamics. 33 (5): 1683. Bibcode:2010JGCD...33.1683N. CiteSeerX   10.1.1.622.3859 . doi:10.2514/1.49550. Archived from the original (PDF) on 2011-11-03.
  7. Saito, Y. (2009). "Observation of magnetic field lines in the vicinity of a superconductor with the naked eye". European Journal of Physics . 31 (1): 229–238. arXiv: 0805.3990 . Bibcode:2010EJPh...31..229S. doi:10.1088/0143-0807/31/1/020. S2CID   56360791.

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