High-strength cold-rolled steel sheet having excellent surface quality and low material variation, and method for manufacturing same
US-2024384366-A1 · Nov 21, 2024 · US
US9514869B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9514869-B2 |
| Application number | US-201314378432-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 13, 2013 |
| Priority date | Feb 13, 2012 |
| Publication date | Dec 6, 2016 |
| Grant date | Dec 6, 2016 |
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The present invention provides an R-T-B based sintered magnet including R 2 T 14 B crystal grains wherein; a grain boundary is formed by two or more adjacent R 2 T 14 B crystal grains, an R—O—C concentrated part, in which concentrations of R, O and C are higher than those in the R 2 T 14 B crystal grains respectively, is in the grain boundary, and an area of the R—O—C concentrated part occupying in that of the grain boundary on a cut surface of the R-T-B based sintered magnet is within a range of 10% or more to 75% or less.
Opening claim text (preview).
The invention claimed is: 1. An R-T-B based sintered magnet comprising R 2 T 14 B crystal grains and grain boundaries formed by two or more adjacent R 2 T 14 B crystal grains, wherein: R represents at least one rare earth element; T represents at least one transition metal element comprising Fe or Fe and Co; the grain boundaries comprise R—O—C concentrated parts; the R—O—C concentrated parts are entire areas of the grain boundaries have concentrations of R, O, and C that are higher than concentrations of R, O, and C in the R 2 T 14 B crystal grains; an average area ratio of the total R—O—C concentrated parts to the entire grain boundaries is within a range of 14% or more to 71% or less, and an average ratio (O/R) of O atom to R atom in the R—O—C concentrated parts is within a range of 0.41 or more to 0.70 or less. 2. The R-T-B based sintered magnet as set forth in claim 1 , wherein the R—O—C concentrated parts comprise a cubic crystal structure. 3. The R-T-B based sintered magnet as set forth in claim 2 , wherein the average area ratio of the total R—O—C concentrated parts to the entire grain boundaries is within a range of 35% or more to 71% or less. 4. The R-T-B based sintered magnet as set forth in claim 3 , wherein an oxygen amount included in the R-T-B based sintered magnet is 1940 ppm or less. 5. The R-T-B based sintered magnet as set forth in claim 4 , wherein “R” included in the R—O—C concentrated parts comprise a rare earth element that at least includes either or both of Nd and Pr (RL), and a rare earth element that at least includes either or both of Dy and Tb (RH). 6. The R-T-B based sintered magnet as set forth in claim 1 , wherein a coercivity of the R-T-B based sintered magnet is 1325 kA/m or more. 7. The R-T-B based sintered magnet as set forth in claim 1 , wherein a coercivity of the R-T-B based sintered magnet is 1325 kA/m to 2276 kA/m. 8. The R-T-B based sintered magnet as set forth in claim 1 , wherein a magnetic flux density of the R-T-B based sintered magnet is 1291 mT or more. 9. The R-T-B based sintered magnet as set forth in claim 1 , wherein a magnetic flux density of the R-T-B based sintered magnet is 1291 to 1418 mT. 10. An R-T-B based sintered magnet comprising R 2 T 14 B crystal grains and grain boundaries formed by two or more adjacent R 2 T 14 B crystal grains, wherein: R represents at least one rare earth element; T represents at least one transition metal element comprising Fe or Fe and Co; the grain boundaries comprise R—O—C—N concentrated parts; the R—O—C—N concentrated parts are entire areas of the grain boundaries that have concentrations of R, O, C, and N that are higher than concentrations of R, O, C, and N in the R 2 T 14 B crystal grains; and an average area ratio of the total R—O—C—N concentrated parts to the entire grain boundaries is within a range of 13% or more to 72% or less. 11. The R-T-B based sintered magnet as set forth in claim 10 , wherein an average ratio (O/R) of O atom to R atom in the R—O—C—N concentrated parts is within a range of 0.41 or more to 0.70 or less. 12. The R-T-B based sintered magnet as set forth in claim 11 , wherein the R—O—C—N concentrated parts comprise a cubic crystal structure. 13. The R-T-B based sintered magnet as set forth in claim 12 , wherein the average area ratio of the total R—O—C—N concentrated parts to the entire grain boundaries is within a range of 36% or more to 72% or less. 14. The R-T-B based sintered magnet as set forth in claim 13 , wherein an oxygen amount included in the R-T-B based sintered magnet is 1950 ppm or less. 15. The R-T-B based sintered magnet as set forth in claim 14 , wherein “R” included in the R—O—C—N concentrated parts comprise a rare earth element that at least includes either or both of Nd and Pr (RL), and a rare earth element that at least includes either or both of Dy and Tb (RH). 16. The R-T-B based sintered magnet as set forth in claim 10 , wherein a coercivity of the R-T-B based sintered magnet is 1412 kA/m or more. 17. The R-T-B based sintered magnet as set forth in claim 10 , wherein a coercivity of the R-T-B based sintered magnet is 1412 to 2073 kA/m. 18. The R-T-B based sintered magnet as set forth in claim 10 , wherein a magnetic flux density of the R-T-B based sintered magnet is 1282 mT or more. 19. The R-T-B based sintered magnet as set forth in claim 10 , wherein a magnetic flux density of the R-T-B based sintered magnet is 1282 to 1391 mT.
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