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Geometrical enhancements to permanent magnet flux sources: application to energy efficient magnetocaloric refrigeration systems

S.J. Lee, David C. Jiles

Open publisher page 19 citations

Abstract

The research reported here shows that a magnetic flux density B far in excess of the magnetic remanence B/sub R/ of a permanent magnet material can be achieved by arranging permanent magnets in the form of hollow cylindrical shells (magic rings), or hollow spherical shells (magic spheres) with additional modifications. In this paper, we report on three additional modifications to enhance the magnetic flux density in the pole gap, i) by changing the cross sectional shape of the permanent magnet array into an ellipse instead of a circle, ii) by including a high remanence flux concentrator close to the air gap and iii) by surrounding the magnet array with a soft magnetic shell which acts as a flux return path. In this way flux densities in excess of 3 Tesla can be achieved in a 23.5 mm/sup 2//spl times/15.2 mm pole gap using NdFeB magnets with remanence of only 1.2 Tesla. The enhanced magnetic flux density can be used for magnetic refrigeration systems, which require sources of magnetic field typically above 1.5 Tesla.

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What this paper is about

The research reported here shows that a magnetic flux density B far in excess of the magnetic remanence B/sub R/ of a permanent magnet material can be achieved by arranging permanent magnets in the form of hollow cylindrical shells (magic rings), or hollow spherical shells (magic spheres) with additional modifications. In this paper, we report on three additional modifications to enhance the magnetic flux density in the pole gap, i) by changing the cross sectional shape of the permanent magnet array into an ellipse instead of a circle, ii) by including a high remanence flux concentrator close to the air gap and iii) by surrounding the magnet array with a soft magnetic shell which acts as a flux return path. In this way flux densities in excess of 3 Tesla can be achieved in a 23.5 mm/sup 2//spl times/15.2 mm pole gap using NdFeB magnets with remanence of only 1.2 Tesla. The enhanced magnetic flux density can be used for magnetic refrigeration systems, which require sources of magnetic field typically above 1.5 Tesla.

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Available abstract

The research reported here shows that a magnetic flux density B far in excess of the magnetic remanence B/sub R/ of a permanent magnet material can be achieved by arranging permanent magnets in the form of hollow cylindrical shells (magic rings), or hollow spherical shells (magic spheres) with additional modifications. In this paper, we report on three additional modifications to enhance the magnetic flux density in the pole gap, i) by changing the cross sectional shape of the permanent magnet array into an ellipse instead of a circle, ii) by including a high remanence flux concentrator close to the air gap and iii) by surrounding the magnet array with a soft magnetic shell which acts as a flux return path. In this way flux densities in excess of 3 Tesla can be achieved in a 23.5 mm/sup 2//spl times/15.2 mm pole gap using NdFeB magnets with remanence of only 1.2 Tesla. The enhanced magnetic flux density can be used for magnetic refrigeration systems, which require sources of magnetic field typically above 1.5 Tesla.

Key concepts: Remanence, Magnet, Magnetic flux, Neodymium magnet, Electropermanent magnet, Materials science, Magnetic field, Magnetic refrigeration

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