Strain amplitude-dependent anelasticity in Cu-Ni solid solution due to thermally activated and athermal dislocation-point obstacle interactions

被引:25
作者
Kustov, S [1 ]
Gremaud, G
Benoit, W
Golyandin, S
Sapozhnikov, K
Nishino, Y
Asano, S
机构
[1] Ecole Polytech Fed Lausanne, Inst Genie Atom, CH-1015 Lausanne, Switzerland
[2] AF Ioffe Physicotech Inst, St Petersburg 194021, Russia
[3] Nagoya Inst Technol, Showa Ku, Nagoya, Aichi 466, Japan
基金
美国国家科学基金会;
关键词
D O I
10.1063/1.369276
中图分类号
O59 [应用物理学];
学科分类号
摘要
Experimental investigations of the internal friction and the Young's modulus defect in single crystals of Cu-(1.3-7.6) at. % Ni have been performed for 7-300 K over a wide range of oscillatory strain amplitudes. Extensive data have been obtained at a frequency of vibrations around 100 kHz and compared with the results obtained for the same crystals at a frequency of similar to 1 kHz. The strain amplitude dependence of the anelastic strain amplitude and the average friction stress acting on a dislocation due to solute atoms are also analyzed. Several stages in the strain amplitude dependence of the internal friction and the Young's modulus defect are revealed for all of the alloy compositions, at different temperatures and in different frequency ranges. For the 100 kHz frequency, low temperatures and low strain amplitudes (similar to 10(-7)-10(-5)), the amplitude-dependent internal friction and the Young's modulus defect are essentially temperature independent, and are ascribed to a purely hysteretic internal friction component. At higher strain amplitudes, a transition stage and a steep strain amplitude dependence of the internal friction and the Young's modulus defect are observed, followed by saturation at the highest strain amplitudes employed. These stages are temperature and frequency dependent and are assumed to be due to thermally activated motion of dislocations. We suggest that the observed regularities in the entire strain amplitude, temperature and frequency ranges correspond to a motion of dislocations in a two-component system of obstacles: weak but long-range ones, due to the elastic interaction of dislocations with solute atoms distributed in the bulk of the crystal; and strong short-range ones, due to the interaction of dislocations with solute atoms distributed close to dislocation glide planes. Based on these assumptions, a qualitative explanation is given for the variety of experimental observations. (C) 1999 American Institute of Physics. [S0021-8979(99)03802-5].
引用
收藏
页码:1444 / 1459
页数:16
相关论文
共 60 条
[1]   DISLOCATION-MOTION IN AN IMPURE CRYSTAL .1. STEADY MOTION [J].
ARAKI, H ;
NINOMIYA, T .
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 1976, 41 (05) :1684-1691
[3]   ANALYTICAL EXPRESSIONS OF INTRINSIC INTERNAL-FRICTION BASED ON DAMPING DATA UNDER INHOMOGENEOUS STRAINS [J].
ASANO, S .
PHILOSOPHICAL MAGAZINE, 1974, 30 (05) :1155-1159
[4]   ORIGIN OF THE LOW-FREQUENCY INTERNAL-FRICTION BACKGROUND OF GOLD [J].
BAUR, J ;
BENOIT, W .
JOURNAL OF APPLIED PHYSICS, 1986, 60 (10) :3473-3478
[5]   STUDY OF THE DISLOCATION CONTRIBUTION TO THE INTERNAL-FRICTION BACKGROUND OF GOLD [J].
BAUR, J ;
BENOIT, W .
JOURNAL OF APPLIED PHYSICS, 1987, 61 (07) :2463-2468
[6]   EFFECT OF SUBSTITUTIONAL IMPURITIES ON THE LOW-TEMPERATURE INTERNAL-FRICTION SPECTRUM OF COLDWORKED DILUTED GOLD-ALLOYS [J].
BONJOUR, C ;
BENOIT, W .
ACTA METALLURGICA, 1979, 27 (11) :1755-1764
[8]  
CHELNOKO.VA, 1970, FIZ TVERD TELA+, V12, P649
[9]  
Chelnokov V. A., 1980, Soviet Physics - Solid State, V22, P1751
[10]  
CHENOKOV VA, 1982, SOV PHYS-SOLID STATE, V24, P1796