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Trapped Magnetic Field Experiments and Characterization of Large-Sized Bulk MgB2 Samples

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HAL Id: hal-01281147

https://hal.archives-ouvertes.fr/hal-01281147

Submitted on 2 Mar 2016

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Trapped Magnetic Field Experiments and

Characterization of Large-Sized Bulk MgB2 Samples

Kévin Berger, Bruno Douine, Jacques Noudem, Frédéric Trillaud, Michael Koblischka, Jean Lévêque

To cite this version:

Kévin Berger, Bruno Douine, Jacques Noudem, Frédéric Trillaud, Michael Koblischka, et al.. Trapped Magnetic Field Experiments and Characterization of Large-Sized Bulk MgB2 Samples. 5th Interna- tional Conference on Superconductivity and Magnetism - ICSM2016, Apr 2016, Fethiye, Turkey. p.

182, ID 539. �hal-01281147�

(2)

Trapped Magnetic Field Experiments

and Characterization of Large-Sized Bulk MgB

2

Samples K. Berger

1

, B. Douine

1

, J. Noudem

2,3

,

F. Trillaud

4

, M.R. Koblischka

5

, and J. Lévêque

1

.

1

University of Lorraine, GREEN, 54506 Vandoeuvre-lès-Nancy, France

2

CRISMAT, CNRS/ENSICAEN, 14050 Caen, France

3

Caen University, LUSAC, 50130 Cherbourg-Octeville, France

4

National Autonomous University of Mexico, Institute of Engineering, 04510 Mexico

5

Saarland University, Institute of Experimental Physics, 66123 Saarbrücken, Germany Contact e-mail: kevin.berger@univ-lorraine.fr

From the applications point of view, the advantage of the very low density of MgB

2

bulk samples must be taken into consideration and, the generation of strong magnetic flux densities using MgB

2

should be investigated [1]. In this contribution, we have studied the trapped magnetic field properties of samples of 20 mm, 40 mm and 50 mm in diameter. Samples with a diameter of 20 mm and 40 mm were processed by ex-situ Spark Plasma Sintering, since the sample of 50 mm of diameter, from Edison Spa, has been produced using a Reactive Mg- Liquid Infiltration process. Both processes are able to produce dense and high quality MgB

2

samples. For the sample of 40 mm diameter, some Field Cooling experiments were carried out at temperatures from 10 K to 30 K both on a single pellet of 4 mm high and on a stack of several pellets of the same diameter. With the help of modeling tools, we have simulated the behavior of such samples in order to deduce their parameters as J

c

(B) and n-value, Fig. 1.

Fig. 1: Two models of critical current density (a), and the simulated resulting trapped magnetic field at the center of the surface of a bulk MgB

2

of 20 mm of diameter and 4 mm high (b).

With these simulations and experiments, we will show that the most relevant parameter for the applications of large-sized bulk MgB

2

samples as permanent magnet is the irreversibility field H

irr

and not the critical current density at zero field J

c

(0).

References

1. J. G. Noudem, M. Aburras, P. Bernstein, X. Chaud, M. Muralidhar, and M. Murakami, Development in processing of MgB2 cryo-magnet superconductors, J. Appl. Phys. 116, 163916 (2014).

(a) (b)

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