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COMPOSITES THEORY AND PRACTICE

formerly: KOMPOZYTY (COMPOSITES)

Effect of titanium addition on structure and magnetic properties of hard magnetic Nd-Fe-B nanocomposites

Marzena Spyra, Marcin Leonowicz* Warsaw University of Technology, Faculty of Materials Science and Engineering, Wołoska 141, 02-507 Warsaw, Poland e-mail: * mkl@inmat.pw.edu.pl

Quarterly No. 1, 2007 pages 9-12

DOI:

keywords: hard magnetic nanocomposites, Nd-Fe-B magnets, Nd-Fe-B-Ti magnets

article version pdf (3.71MB)

abstract Among a variety of magnetic materials, in early 90 s of the XXth century, appeared a new class of alloys called magnetic nanocomposites. Such materials combine hard and soft nanostructured magnetic phases giving rise for the property enhan¬cement. These materials take advantage of the correlations between the exchange and anisotropy energy. When the grains are small enough (for the Nd-Fe-B magnets this critical size is close to 30 nm) the exchange length L from crystallites oriented favourably with their easy magnetisation axes to the external magnetic field, covers substantial part of the neighbouring gra-ins. The exchange length is proportional to the exchange constant A and reversibly proportional to average anisotropy con-stant . The latter coefficient strongly depends on the grain size dz. Thus, in nanocrystalline magnets the exchange length covers substantial volume of neighbouring crystallites. As a result the material gains some proportion of magnetic anisotropy in a crystallographically isotropic state. In this study the nanocomposite Nd9Fe77-xB14Tix system, containing hard magnetic Nd2Fe14B phase and soft magnetic Fe phase, was investigated. The effect of titanium addition on the structure and magnetic properties was studied. It was found that 24 at. % Ti addition leads to substantial increase of the coercivity and maximum energy product maintaining the remanence unchanged. The highest properties: Jr = 0.81 T, JHc = 907 kA/m, (BH)max = = 99 kJ/m3 have been achieved for the Nd9Fe73B14Ti4 alloy. This effect we attribute to the fine and homogeneous grain struc-ture in Ti containing materials. The hysteresis loops for Ti containing alloys are smooth and characteristic of a single phase alloys. The initial magnetization curve indicates change of the coercivity mechanisms giving rise to pinning of domain walls, which is caused by the reduction of the crystallite size.

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