INVESTIGATIONS ON THERMAL STABILITY OF FATIGUE DISLOCATION STRUCTURES IN CONJUGATE AND CRITICAL DOUBLE-SLIP-ORIENTED Cu SINGLE CRYSTALS

doi:10.11900/0412.1961.2015.00572

Acta Metall Sin

2016, Vol. 52

Issue (6): 761-768 DOI: 10.11900/0412.1961.2015.00572

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INVESTIGATIONS ON THERMAL STABILITY OF FATIGUE DISLOCATION STRUCTURES IN CONJUGATE AND CRITICAL DOUBLE-SLIP-ORIENTED Cu SINGLE CRYSTALS

Weiwei GUO¹(

),Chengjun QI¹,Xiaowu LI^1,²

1 Institute of Materials Physics and Chemistry, School of Materials Science and Engineering, Northeastern University, Shenyang 110819, China
2 Key Laboratory for Anisotropy and Texture of Materials, Ministry of Education, Northeastern University, Shenyang 110819, China

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Weiwei GUO,Chengjun QI,Xiaowu LI. INVESTIGATIONS ON THERMAL STABILITY OF FATIGUE DISLOCATION STRUCTURES IN CONJUGATE AND CRITICAL DOUBLE-SLIP-ORIENTED Cu SINGLE CRYSTALS. Acta Metall Sin, 2016, 52(6): 761-768.

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Abstract

It is well known that the cyclic deformation behavior and dislocation structures of Cu single crystals with different orientations have been systematically investigated and understood. However, there is as yet no general and unequivocal knowledge of the thermal stability of fatigue-induced dislocation structures in Cu single crystals, which is particularly significant for the further improvement of low energy dislocation structure (LEDS) theory. In previous work, the thermal stability of fatigue dislocation structures in 18 41] single-slip and coplanar double-slip Cu single crystals have been reported. For deeply understanding the orientation-dependent thermal stability of fatigue dislocation structures, in the present work, conjugate and [017] critical double-slip-oriented Cu single crystals were cyclically deformed at different plastic strain amplitudes γ_plup to saturation, and then annealed at different temperatures (300, 500 and 800 ℃) for 30 min, to examine the thermal stability of various fatigue-induced dislocation structures. It was found that an obvious recovery has occurred in various dislocation structures at 300 ℃. At the higher temperatures, e.g., 500 and 800 ℃, a remarkable recrystallization phenomenon takes place together with the formation of many annealing twins. The thermal stability of various dislocation structures produced in fatigued Cu single crystals with different orientations from high to low are on the order of vein structure, persistent slip band (PSB) structure, labyrinth structure and dislocation cells. The annealing twins formed in Cu single crystals with different orientations all develop strictly along the dislocation slip planes, which have been operated under fatigue deformation. The more serious the fatigue-induced slip deformation, the greater the amount of annealing twins would be. Furthermore, an over high annealing temperature, e.g. 800 ℃, would greatly speed up the migration of boundaries of recrystallized grains to restrain the formation of annealing twins, leading to, more or less, the decrease in the amount of twins.

Key words: Cu single crystal fatigue dislocation structure thermal stability crystallographic orientation recrystallization annealing twin

Received: 09 November 2015

Fund: Supported by National Natural Science Foundation of China (Nos.51071041, 51231002, 51271054 and 51571058) and Specialized Research Fund for the Doctoral Program of Higher Education of China (No.20110042110017)

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	Weiwei GUO
	Chengjun QI
	Xiaowu LI

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https://www.ams.org.cn/EN/10.11900/0412.1961.2015.00572 OR https://www.ams.org.cn/EN/Y2016/V52/I6/761

Table1 Fatigue testing conditions and data for and [017] Cu single crystals

Fig.1 SEM-ECC images of dislocation structures in cyclically deformed Cu single crystals at γ_pl=1.5×10^-4 (a, b), and microstructures formed after subsequent annealing at 300 ℃ (c), 500 ℃ (d) and 800 ℃ (e, f) for 30 min (All observed planes are parallel to the loading direction, PSB—persistent slip band, GB—grain boundary)

Fig.2 SEM-ECC images of dislocation structures in cyclically deformed Cu single crystals at γ_pl=1.5×10^-3 (a, b), and microstructures formed after subsequent annealing at 300 ℃ (c), 500 ℃(d, e) and 800 ℃ (f) for 30 min (All observed planes are parallel to the loading direction)

Fig.3 SEM-ECC images of dislocation structures in cyclically deformed [017] Cu single crystals at γ_pl=6.5×10^-3 (a, b), and microstructures formed after subsequent annealing at 300 ℃ (c), 500 ℃ (d, e) and 800 ℃ (f) for 30 min (The observed planes are parallel to the loading direction except for Fig.3e, for which the observed plane is perpendicular to the loading direction)

Fig.4 TEM images of microstructures formed after subsequent annealing for 30 min in cyclically deformed Cu single crystals at γ_pl=1.5×10^-4 at 500 ℃, B=[110] (a), and 800 ℃, B=[114] (b) (B—the incident electron-beam direction)

Fig.5 TEM images of microstructures formed after subsequent annealing for 30 min in cyclically deformed Cu single crystals at γ_pl =1.5×10^-3 at 500 ℃, B=[211] (a, b), 800 ℃, B=[223] (c), and 800 ℃, B=[110] (d)

Fig.6 TEM images of microstructures formed after subsequent annealing for 30 min in cyclically deformed [017] Cu single crystals at γ_pl=6.5×10^-4 at room temperature (RT), B=[421] (a), 300 ℃, B=[100] (b), 500 ℃, B=[110] (c, d), and 800 ℃, B=[110] (e, f) (Inset in Fig.6f shows the SAED pattern of the twin)

Fig.7 Typical DSC plots for cyclically saturated [017] Cu single crystal at γ_pl= 6.5×10^-3

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