2001
DOI: 10.1109/20.951221
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Coercivity of titanium-substituted high-temperature permanent magnets

Abstract: Abstract-The temperature dependence of the coercivity of Sm-Co based magnets is investigated by magnetization measurements and model calculations. The Zr-free titanium-substituted Sm-Co material exhibits a positive temperature coefficient of the coercivity (TCC) above room temperature, a reasonable hysteresis-loop shape, and an appreciable coercivity of 12.3 kOe at 500 C for the nominal composition Sm(Co 6 2 Cu 0 8 Ti 0 3 ). The samples were produced by heat-treating the disordered 1 : 5 alloy commonly referre… Show more

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Cited by 25 publications
(17 citation statements)
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“…This is due to the different temperature dependence of the two phases (1:5 and 2:17). A detailed explanation of this mechanism has been given elsewhere [4]. Figure 3(a) shows the room-temperature loop of a sample, whereas 3(b) shows the same sample after alignment.…”
Section: Resultsmentioning
confidence: 99%
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“…This is due to the different temperature dependence of the two phases (1:5 and 2:17). A detailed explanation of this mechanism has been given elsewhere [4]. Figure 3(a) shows the room-temperature loop of a sample, whereas 3(b) shows the same sample after alignment.…”
Section: Resultsmentioning
confidence: 99%
“…On further addition of Fe, the TCC becomes negative and also the coercivity drops to a relatively low level. The positive TCC has been explained by a model in terms of domain-wall-pinning mechanism in a two-phase magnet [4]. As in the case of conventional SmCo 2:17 magnets, Fe substitutes for Co and most likely enters the main 2:17 phase in the cellular structure, and also stabilizes the 2:17 phase at the presence of Cu [5].…”
Section: Resultsmentioning
confidence: 99%
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“…In the last couple of years efforts have been made to improve the properties of this class of material by adjusting the composition and Hc values up to 10 kOe have been obtained at 500 'C [I]. Recently we have discovered a relatively simple Sm-Co-Cu-Ti alloy that consists of two phases, 2:17 and 1:5, and which has a positive dHc/dT and H, values above 10 kOe at 500 'C [2,3]. We discuss here our most recent improvements in this material and our understanding of its behavior.…”
Section: Sm-co-cu-ti Hybrid Bulk Magnetsmentioning
confidence: 99%
“…where Ho is the anisotropy field of the main (2:17) phase, Kh is the anisotropy constant of same phase, b is the thickness of the boundary (1:5) phase, 5 is the domain-wall thickness, and AK = Kh -K, where Ks is the anisotropy of the softer boundary phase [3]. By considering the expected temperature dependence of Kh and K, and the expected dependence of Ks on Cu content, it is possible to rationalize the temperature dependence of H-(T) shown in Figure 5, including the maximum in H,(T) seen for the sample with x = 0.6.…”
Section: Sm-co-cu-ti Hybrid Bulk Magnetsmentioning
confidence: 99%