Grain boundary diffusion process for rare-earth magnets
US-9786419-B2 · Oct 10, 2017 · US
US11830645B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11830645-B2 |
| Application number | US-202016732426-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jan 2, 2020 |
| Priority date | Jul 5, 2017 |
| Publication date | Nov 28, 2023 |
| Grant date | Nov 28, 2023 |
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A manufacturing method of a sintered magnet is described. The method includes forming a pre-sintering body from a first magnetic powder and a second magnetic powder (containing a heavy rare earth element, HRE) so that at least part of the second magnetic powder is provided at at least one inner portion of the pre-sintering body and surrounded format least two opposite sides by the first magnetic powder; sintering the pre-sintering body; and annealing the sintered pre-sintering body at an annealing temperature lower than the sintering temperature, thereby causing inter-grain diffusion of HRE from the HRE reservoir zone to the grain boundary phase. After the annealing, the grain boundary phase contains the HRE in a higher concentration than the main phase.
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The invention claimed is: 1. A manufacturing method of a sintered magnet, the method comprising: forming a pre-sintering body from a first magnetic powder and a second magnetic powder so that at least part of the second magnetic powder is provided on at least one inner portion of the pre-sintering body and surrounded from at least two opposite sides by the first magnetic powder, wherein the first magnetic powder has an R-T-B structure, wherein R is at least one selected from the group consisting of Y, Ce, La, Pr, Nd, Sm, Eu and Gd, and T is one or more transition metal elements including Fe, wherein the second magnetic powder contains at least one heavy rare earth element (HRE), wherein a melting temperature T M1 of the first magnetic powder is higher than a melting temperature T M2 of the second magnetic powder, the pre-sintering body having a thickness of at least 6 mm; sintering the pre-sintering body at a temperature T s being higher than the melting temperature T M2 of the second magnetic powder and lower than the melting temperature T M1 of the first magnetic powder, thereby creating a main phase of grains from the first magnetic powder with a grain boundary phase in-between the grains, and an HRE reservoir zone from the second magnetic powder, wherein the sintering is Spark Plasma Sintering; and annealing the sintered pre-sintering body at an annealing temperature T A lower than the sintering temperature T s , thereby causing inter-grain diffusion of HRE from the HRE reservoir zone to the grain boundary phase so that after the annealing the grain boundary phase contains at least one heavy rare earth element (HRE) in a higher concentration than the main phase. 2. The method according to claim 1 , wherein the R-T-B structure is a Nd—Fe—B structure. 3. The method according to claim 1 , wherein the at least one heavy rare earth element (HRE) comprises Dy or Tb. 4. The method according to claim 1 , wherein the second magnetic powder is a eutectic or near-eutectic alloy. 5. The method according to claim 1 , wherein the melting temperature T M1 of the first magnetic powder is higher than the melting temperature T M2 of the second magnetic powder by at least 20° C. 6. The method according to claim 1 , wherein the second magnetic powder is provided in a plurality of HRE reservoir zones of the pre-sintering body, the plurality of HRE reservoir zones being each surrounded from at least two opposite sides by the first magnetic powder. 7. The method according to claim 6 , wherein the plurality of HRE reservoir zones are spaced apart from each other by at most 6 mm. 8. The method according to claim 6 , wherein at least one of the plurality of HRE reservoir zones is located at a depth of at least 3 mm from a nearest surface of the pre-sintering body. 9. The method according to claim 1 , wherein T M2 ≤T A +10° C. 10. The method according to claim 1 , wherein an annealing time and annealing temperature T A is set for inter-grain diffusion of a major part of the HRE from the HRE reservoir zone to the grain boundary phase. 11. The method according to claim 1 , wherein the annealing temperature T A is set lower than the sintering temperature T s , and/or higher than the melting temperature T M2 of the second magnetic powder. 12. The method according to claim 2 , wherein the at least one heavy rare earth element (HRE) comprises Dy or Tb. 13. The method according to claim 12 , wherein the second magnetic powder is a eutectic or near-eutectic alloy. 14. The method according to claim 13 , wherein the melting temperature T M1 of the first magnetic powder is higher than the melting temperature T M2 of the second magnetic powder by at least 20° C. 15. The method according to claim 2 , wherein the second magnetic powder is a eutectic or near-eutectic alloy. 16. The method according to claim 2 , wherein the second magnetic powder is provided in a plurality of HRE reservoir zones of the pre-sintering body, the plurality of HRE reservoir zones being each surrounded from at least two opposite sides by the first magnetic powder. 17. The method according to claim 16 , wherein the plurality of HRE reservoir zones are spaced apart from each other by at most 6 mm. 18. The method according to claim 16 , wherein at least one of the plurality of HRE reservoir zones is located at a depth of at least 3 mm from a nearest surface of the pre-sintering body. 19. The method according to claim 2 , wherein the annealing temperature T A is set lower than the sintering temperature T s , and/or higher than the melting temperature T M2 of the second magnetic powder. 20. The method according to claim 2 , wherein the HRE reservoir zone is located at a depth of at least 3 mm from a nearest surface of the pre-sintering body; and wherein T M2 ≤T A +10° C. 21. The method according to claim 1 , wherein the second magnetic powder is provided in a plurality of HRE reservoir zones of the pre-sintering body, wherein the HRE reservoir zones are spaced apart from each other by at most 3 mm. 22. The method according to claim 1 , wherein T M2 ≤T A . 23. The method according to claim 2 , wherein T M2 ≤T A . 24. The method according to claim 16 , wherein the plurality of HRE reservoir zones are spaced apart from each other by at most 3 mm.
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