Damping characteristics of TiNi shape memory alloys

The damping characteristics of TiNi SMAs have been systematically studied by using techniques of resonant-bar and low-frequency inverted torsion pendulum. Experimental results show that both the martensite phase (M) and R phase (R) have high damping due to the movement of twin boundaries. Because the B2 parent phase (B2) has smaller damping, it is suggested that this may come from the dynamic ordering process of lattice defects. In the transformation re-gions of B2 ↔ M, B2 ↔ R, and R ↔ M, there are maxima of the damping capacity which are attributed to two contributions. One arises from the plastic strain and twin-interface move-ment during the thermal transformation, which obeys a linear variation of peak heightsQ−1max vst att ≥ 1 °C/min. The other originates from the stress-induced transformation formed by the applied external stress which dominates atT < 1 °C/min. The elastic modulusE of martensite and the R phase is lower than that of the B2 phase, and a modulus minimum appears in the transformation region.

[1]  Shuichi Miyazaki,et al.  Deformation and transition behavior associated with theR-phase in Ti-Ni alloys , 1986 .

[2]  K. N. Melton,et al.  The mechanical properties of NiTi-based shape memory alloys , 1981 .

[3]  C. M. Wayman,et al.  The R-phase transition and associated shape memory mechanism in Ti-Ni single crystals , 1988 .

[4]  R. Batist Internal Friction of Structural Defects in Crystalline Solids , 1972 .

[5]  Hsin-Chih Lin,et al.  A study of electrical resistivity, internal friction and shear modulus on an aged Ti49Ni51 alloy , 1990 .

[6]  R. Hasiguti,et al.  Effect of Preannealings on the Temperature Spectra of Internal Friction and Shear Modulus of Ti–51Ni , 1987 .

[7]  B. Darinskii,et al.  Internal friction at first-order phase transitions in solids , 1976 .

[8]  B. S. Berry,et al.  Anelastic Relaxation in Crystalline Solids , 1972 .

[9]  P. Ossi Theory of thermoelastic martensite nucleation , 1986 .

[10]  D. W. James High damping metals for engineering applications , 1969 .

[11]  O. Mercier,et al.  Low-frequency internal friction peaks associated with the martensitic phase transformation of NiTi , 1979 .

[12]  Jinsong Zhu,et al.  Internal friction transitory effects associated with martensitic transformation in NiTi alloys , 1988 .

[13]  S. Etienne,et al.  New Aspects of Internal Friction during Martensitic Transformation of a Cu–Zn–Al Alloy , 1981 .

[14]  K. Sugimoto,et al.  Simultaneous measurements of internal friction, young's modulus and shape change associated with thermoelastic martensite transformation in CuAlNi single crystals , 1974 .

[15]  Z. L. Pan,et al.  High-damping metals and alloys , 1991 .

[16]  Huibin Xu,et al.  On the pseudo-elastic hysteresis , 1991 .

[17]  Yoshiyuki Nakata,et al.  Thermal Cycling Effects in an Aged Ni-rich Ti–Ni Shape Memory Alloy , 1987 .

[18]  L. Delaey,et al.  FACTORS AFFECTING INTERNAL-FRICTION PEAK DUE TO THERMOELASTIC MARTENSITIC-TRANSFORMATION , 1976 .

[19]  A. E. Schwaneke,et al.  Magnetic Susceptibility and Internal Friction of Tetragonal Manganese‐Copper Alloys Containing 70 Percent Manganese , 1962 .

[20]  Tae-Hyun Nam,et al.  Shape Memory Characteristics Associated with the B2\ightleftarrowsB19 and B19\ightleftarrowsB19′ Transformations in a Ti-40Ni-10Cu (at.%) Alloy , 1990 .

[21]  H. Horng,et al.  A study of B2↔B19↔B19′ two-stage martensitic transformation in a Ti50Ni40Cu10 alloy , 1993 .