TY - JOUR
T1 - A novel two-step grain boundary diffusion process using TaF5 and Pr70Cu15Al10Ga5 for realizing high-coercivity in Nd-Fe-B-sintered magnets without use of heavy rare-earth
AU - Lee, Seol mi
AU - Kim, Ganghwi
AU - Lee, Ki Suk
AU - Kim, Sumin
AU - Kim, Tae Hoon
AU - Lee, Sang hyub
AU - Kim, Dong Hwan
AU - Lee, Wooyoung
AU - Lee, Jung Goo
N1 - Publisher Copyright:
© 2024 The Author(s)
PY - 2025/2/15
Y1 - 2025/2/15
N2 - To achieve high-coercivity in Nd-Fe-B-sintered magnets without relying on the use of heavy rare-earth (HRE), developing an HRE-free grain-boundary-diffusion-process (GBDP) using the light rare-earth, Pr, is highly desired. The key factor for achieving high-coercivity via Pr-GBDP is to increase the Pr-concentration of Pr-rich shell by reducing its thickness, and this can be realized by inhibiting the chemically induced liquid film migration (CILFM) that occurs to form the shell. Herein, for the first time, we report achievement of high-coercivity of 2.35 T without using HRE by developing CILFM-inhibited two-step GBDP that uses TaF5 to form a intergranular precipitate (PPT) and Pr70Cu15Al10Ga5 to form a Pr-rich shell in the 1st- and 2nd-steps, respectively. Due to the formation of hexagonal-TaB2 intergranular PPT during the 1st-GBDP, the CILFM is inhibited during the 2nd-GBDP, thereby reducing the grain size and forming the thinner shell with higher Pr-concentration in the magnets. As a result, the μ0Hc of two-step GBDP magnets (2.35 T) is considerably higher than that of magnets GBD-treated with Pr70Cu15Al10Ga5 alone (1.85 T). A micromagnetic simulation shows that the nucleation field at the interface between the 2–14–1 grain and Nd-rich phase in two-step GBDP magnets increases by such a thinner and higher Pr-concentration shell. Furthermore, due to the CILFM inhibition, the number of Pr atoms consumed for the shell formation near the magnet surface reduces in the two-step GBDP magnets, resulting in an increased GBD-depth of Pr, and this is another contributor for realizing a high-coercivity in magnets via the HRE-free two-step GBDP.
AB - To achieve high-coercivity in Nd-Fe-B-sintered magnets without relying on the use of heavy rare-earth (HRE), developing an HRE-free grain-boundary-diffusion-process (GBDP) using the light rare-earth, Pr, is highly desired. The key factor for achieving high-coercivity via Pr-GBDP is to increase the Pr-concentration of Pr-rich shell by reducing its thickness, and this can be realized by inhibiting the chemically induced liquid film migration (CILFM) that occurs to form the shell. Herein, for the first time, we report achievement of high-coercivity of 2.35 T without using HRE by developing CILFM-inhibited two-step GBDP that uses TaF5 to form a intergranular precipitate (PPT) and Pr70Cu15Al10Ga5 to form a Pr-rich shell in the 1st- and 2nd-steps, respectively. Due to the formation of hexagonal-TaB2 intergranular PPT during the 1st-GBDP, the CILFM is inhibited during the 2nd-GBDP, thereby reducing the grain size and forming the thinner shell with higher Pr-concentration in the magnets. As a result, the μ0Hc of two-step GBDP magnets (2.35 T) is considerably higher than that of magnets GBD-treated with Pr70Cu15Al10Ga5 alone (1.85 T). A micromagnetic simulation shows that the nucleation field at the interface between the 2–14–1 grain and Nd-rich phase in two-step GBDP magnets increases by such a thinner and higher Pr-concentration shell. Furthermore, due to the CILFM inhibition, the number of Pr atoms consumed for the shell formation near the magnet surface reduces in the two-step GBDP magnets, resulting in an increased GBD-depth of Pr, and this is another contributor for realizing a high-coercivity in magnets via the HRE-free two-step GBDP.
KW - Chemically induced liquid film migration
KW - Grain boundary diffusion process
KW - Heavy rare-earth-free
KW - Intergranular precipitates
KW - Nd-Fe-B-sintered magnets
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U2 - 10.1016/j.actamat.2024.120660
DO - 10.1016/j.actamat.2024.120660
M3 - Article
AN - SCOPUS:85212936038
SN - 1359-6454
VL - 285
JO - Acta Materialia
JF - Acta Materialia
M1 - 120660
ER -