TY - JOUR
T1 - Effects of thermal ε martensite content and deformation on damping capacity of a Co-32 wt.% Ni alloy
AU - Lee, Young Kook
AU - Ha, Tae Joong
AU - Jun, Joong Hwan
AU - Choi, Chong Sool
PY - 2004/4/15
Y1 - 2004/4/15
N2 - The damping capacity of Co-32 wt.% Ni alloy was investigated as a function of the amount of thermal and strain-induced ε martensite under non-magnetic and 900 Oe magnetic fields, respectively. The damping capacity of the Co-32 wt.% Ni alloy containing ε martensite without magnetic field consists of the magneto-mechanical damping capacity of mainly α phase, damping capacities of α and ε phases without magneto-mechanical damping effect. Under a magnetic field of 900 Oe, the more the thermal ε martensite mass fraction the higher the damping capacity. However, the damping capacity of the deformed Co-32 wt.% Ni alloy with the strain-induced ε martensite decreases with increasing deformation degree despite the increase in total ε martensite fraction, because the lattice defects like dislocations introduced during deformation act as barriers to movement of damping sources such as magnetic domain walls, stacking faults boundaries in both α and ε phases, and α/ε interfaces.
AB - The damping capacity of Co-32 wt.% Ni alloy was investigated as a function of the amount of thermal and strain-induced ε martensite under non-magnetic and 900 Oe magnetic fields, respectively. The damping capacity of the Co-32 wt.% Ni alloy containing ε martensite without magnetic field consists of the magneto-mechanical damping capacity of mainly α phase, damping capacities of α and ε phases without magneto-mechanical damping effect. Under a magnetic field of 900 Oe, the more the thermal ε martensite mass fraction the higher the damping capacity. However, the damping capacity of the deformed Co-32 wt.% Ni alloy with the strain-induced ε martensite decreases with increasing deformation degree despite the increase in total ε martensite fraction, because the lattice defects like dislocations introduced during deformation act as barriers to movement of damping sources such as magnetic domain walls, stacking faults boundaries in both α and ε phases, and α/ε interfaces.
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U2 - 10.1016/j.msea.2003.05.005
DO - 10.1016/j.msea.2003.05.005
M3 - Article
AN - SCOPUS:1842737437
SN - 0921-5093
VL - 370
SP - 468
EP - 472
JO - Materials Science & Engineering A: Structural Materials: Properties, Microstructure and Processing
JF - Materials Science & Engineering A: Structural Materials: Properties, Microstructure and Processing
IS - 1-2
ER -