skip to main content
OSTI.GOV title logo U.S. Department of Energy
Office of Scientific and Technical Information

Title: Temperature dependence of coercivity in melt-spun and die upset neodymium-iron-boron

Journal Article · · Journal of Applied Physics; (USA)
DOI:https://doi.org/10.1063/1.344775· OSTI ID:6837248
;  [1]
  1. Physics Department, General Motors Research Laboratories, Warren, Michigan 48090-9055 (USA)

We compare the temperature dependence of the intrinsic coercivity {ital H}{sub {ital ci}} between 5 and 600 K in rapidly quenched Nd-Fe-B ribbons and a die upset Nd-Fe-B magnet. At room temperature, ribbons have higher coercivity than the die upset magnet, but have a smaller technical temperature coefficient of coercivity {beta} between 25 and 125 {degree}C: {ital H}{sub {ital ci}}=15.1 kOe and {beta}={minus}0.38%/{degree}C for the ribbons, while {ital H}{sub {ital ci}}=10.4 kOe and {beta}={minus}0.64%/{degree}C for the die upset magnet. Because the die upset magnet has a stronger temperature dependence, the {ital H}{sub {ital ci}}({ital T}) curves converge at low temperature. The ribbons can be phenomenologically modeled using {ital H}{sub {ital ci}}({ital T})={ital cH}{sub {ital A}}({ital T}){minus}{ital N}{sub eff}4{pi}{ital M}{sub {ital s}}({ital T}), the two terms representing the strength of domain wall pinning at grain boundaries and the effective local demagnetizing field, respectively. The model parameters {ital c}=0.25 and {ital N}{sub eff}=0.26 are significantly smaller than the corresponding values obtained in sintered Nd-Fe-B magnets. This model is less successful in describing {ital H}{sub {ital ci}}({ital T}) for the die upset magnet. Their qualitatively different behaviors indicate that different mechanisms of domain wall pinning are responsible for coercivity in ribbons and die upset magnets.

OSTI ID:
6837248
Journal Information:
Journal of Applied Physics; (USA), Vol. 67:9; ISSN 0021-8979
Country of Publication:
United States
Language:
English