HARD MAGNETIC-PROPERTIES OF BULK AMORPHOUS-ALLOYS

The amorphous phase in the Nd-Fe-Al and Pr-Fe-Al systems is formed in extremely wide composition ranges of 0 to 90 at% Fe and 0 to 93 at% Al by melt spinning. Ferromagnetic Ln(90-x)Fe(x)Al(10) (Ln=Nd or Pr) bul k amorphous alloys with high coercive force at room temperature are ob tained by a copper mold casting method. The maximum diameter of the cy lindrical amorphous samples is 12 mm for the Nd-30%Fe-Al alloy and 3 m m for the Pr-30%Fe-Al alloys and decreases with deviating Fe content. Neither glass transition nor supercooled liquid region is observed in the temperature range before crystallization (T < T-x), which is diffe rent from other bulk amorphous alloys exhibiting wide supercooled liqu id regions. The extremely high T-x/T-n and small Delta T-m(=T-m-T-x) v alues are the reason for the achievement of large glass-forming abilit y in these systems. The bulk amorphous Ln(60)Fe(30)Al(10) alloys are f erromagnetic with the Curie temperature (T-c) of 515 to 600 K which ar e much higher than those for Nd-Fe and Pr-Fe binary amorphous ribbons. The remanence (B-r) and intrinsic coercive force (H-i(c)) are 0.089 t o 0.122 T and 277 to 321 kA/m, respectively, and the crystallization t o Ln+Al(2)Ln+delta phases causes a ferromagnetic- to -paramagnetic pha se transition. Thus, the hard magnetic properties are achieved only in the amorphous state.