Experimental simulation of a magnetic refrigeration cycle in high magnetic fields
- Authors: Dilmieva E.T.1, Kamantsev A.P.1,2, Koledov V.V.1,2, Mashirov A.V.1,2, Shavrov V.G.1, Cwik J.1,2, Tereshina I.S.2,3
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Affiliations:
- Kotelnikov Institute of Radio-Engineering and Electronics
- International Laboratory of High Magnetic Fields and Low Temperatures
- Baikov Institute of Metallurgy and Materials Science
- Issue: Vol 58, No 1 (2016)
- Pages: 81-85
- Section: Magnetism
- URL: https://ogarev-online.ru/1063-7834/article/view/196787
- DOI: https://doi.org/10.1134/S1063783416010108
- ID: 196787
Cite item
Abstract
The complete magnetic refrigeration cycle has been simulated on a sample of gadolinium in magnetic fields of a Bitter coil magnet up to 12 T. The total change of temperature of the sample during the cycle is a consequence of magnetic refrigeration, and the dependence of the magnetization of the sample on the magnetic field exhibits a hysteretic behavior. This makes it possible to determine the work done by the magnetic field on the sample during the magnetic refrigeration cycle and to calculate the coefficient of performance of the process. In a magnetic field of 2 T near the Curie temperature of gadolinium, the coefficient of performance of the magnetic refrigeration is found to be 92. With an increase in the magnetic field, the coefficient of performance of the process decreases sharply down to 15 in a magnetic field of 12 T. The reasons, for which the coefficient of performance of the magnetic refrigeration is significantly below the fundamental limitations imposed by the reversed Carnot theorem, have been discussed.
About the authors
E. T. Dilmieva
Kotelnikov Institute of Radio-Engineering and Electronics
Author for correspondence.
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009
A. P. Kamantsev
Kotelnikov Institute of Radio-Engineering and Electronics; International Laboratory of High Magnetic Fields and Low Temperatures
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009; ul. Gajowicka 95, Wroclaw, 53-421
V. V. Koledov
Kotelnikov Institute of Radio-Engineering and Electronics; International Laboratory of High Magnetic Fields and Low Temperatures
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009; ul. Gajowicka 95, Wroclaw, 53-421
A. V. Mashirov
Kotelnikov Institute of Radio-Engineering and Electronics; International Laboratory of High Magnetic Fields and Low Temperatures
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009; ul. Gajowicka 95, Wroclaw, 53-421
V. G. Shavrov
Kotelnikov Institute of Radio-Engineering and Electronics
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009
J. Cwik
Kotelnikov Institute of Radio-Engineering and Electronics; International Laboratory of High Magnetic Fields and Low Temperatures
Email: kelvit@mail.ru
Russian Federation, ul. Mokhovaya 11–7, Moscow, 125009; ul. Gajowicka 95, Wroclaw, 53-421
I. S. Tereshina
International Laboratory of High Magnetic Fields and Low Temperatures; Baikov Institute of Metallurgy and Materials Science
Email: kelvit@mail.ru
Poland, ul. Gajowicka 95, Wroclaw, 53-421; Leninskii pr. 49, Moscow, 119991
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