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Phase Transformations in Nd–Fe–B-Based Alloys under High Pressure Torsion at Different Temperatures
In this work, we studied the behavior of the Nd–Dy–Fe–Co–Cu–B alloy for permanent magnets under high pressure torsion (HPT). In the initial state of the studied alloy, it mainly contained the crystalline phase τ 1 (Nd, Dy) 2 (Fe, Co, Cu) 14 B. After HPT at room temperature ( T HPT = 30°C), a mixture...
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Published in: | JETP letters 2020-07, Vol.112 (1), p.37-44 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | In this work, we studied the behavior of the Nd–Dy–Fe–Co–Cu–B alloy for permanent magnets under high pressure torsion (HPT). In the initial state of the studied alloy, it mainly contained the crystalline phase τ
1
(Nd, Dy)
2
(Fe, Co, Cu)
14
B. After HPT at room temperature (
T
HPT
= 30°C), a mixture of an amorphous phase with nanocrystalline inclusions of the τ
1
phase is observed in the alloy. In the equilibrium phase diagram, this state is equivalent to a mixture of the τ
1
phase with the melt at the temperature
T
eff
= ∼1100°C. The thus determined
T
eff
value is called the effective temperature. When the
T
HPT
temperature of the HPT treatment increases to 300 and 400°C, the amorphous phase disappears, and the Fe
2
B and γ-Fe phases appear instead. In the equilibrium phase diagram, this state is equivalent to a mixture of phases τ
1
+
Fe
2
B
+
γ-Fe, which is observed in the temperature range from ∼950 to ∼1050°C. We explain this phenomenon by the fact that with an increase in the HPT temperature
T
HPT
, the rate of formation of defects during deformation remains constant, but the rate of their thermal relaxation (annihilation) increases. This is equivalent to decrease in the effective temperature
T
eff
in the equilibrium phase diagram. The previously predicted decrease in
T
eff
with an increase in
T
HPT
is observed for the first time. |
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ISSN: | 0021-3640 1090-6487 |
DOI: | 10.1134/S0021364020130020 |