PROPERTIES AND APPLICATIONS OF HIGH ... - Vacuumschmelze
PROPERTIES AND APPLICATIONS OF HIGH ... - Vacuumschmelze
PROPERTIES AND APPLICATIONS OF HIGH ... - Vacuumschmelze
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[5]. The irreversible polarization losses ∆Jirr due to the temperature dependence of the coercivity HcJ<br />
and due to the thermal aftereffect can be recovered by remagnetization.<br />
TC(B r ) =<br />
TC(H cJ ) =<br />
in %/K, T 0 < T < T 1<br />
20°C 60°C 80°C<br />
100°C<br />
-20 -15 -10 -5 0<br />
magnetic field strength H in kA/cm<br />
120°C<br />
Figure 3: Dependence of the demagnetization curves J(H) and B(H) of VACODYM ®*) 722 HR magnets on the<br />
temperature. The typical magnetic properties amount to: Br = 1.47 T, HcJ = 9.5 kA/cm, (BH)max = 415 kJ/m³ at 20 °C.<br />
rel. polarization losses dJ irr/J in %<br />
0<br />
-5<br />
-10<br />
-15<br />
-20<br />
-25<br />
Nd 14.3DyFe 76.7B 8 magnets<br />
Aging temperature: 130 °C<br />
1 10 100 1000 10000<br />
exposure time in h<br />
B/µoH = -2.0<br />
B/µoH = -1.1<br />
B/µoH = -0.5<br />
Fig. 4: Irreversible polarization losses of sintered Nd14.3DyFe76.7B8 magnets with different load lines B/µoH at a<br />
temperature of 130 °C in dependence of the exposition time.<br />
® registered trade mark of VACUUMSCHMELZE GmbH & Co. KG, *) licenser Sumitomo Special Metals Corp.<br />
1,6<br />
1,2<br />
0,8<br />
0,4<br />
0,0<br />
-0,4<br />
-0,8<br />
polarization J, induction B in T