Acta Physica Sinica, Volume. 68, Issue 24, 246102-1(2019)

Molecular dynamics simulation of effect of temperature on void nucleation and growth of single crystal iron at a high strain rate

Yun-Tian Wang, Xiang-Guo Zeng*, and Xin Yang
Figures & Tables(18)
Model of single crystal iron under triaxial tension (atoms are colored by CNA).单晶铁三轴拉伸模型
Tensile stress as a function of time at 100–1100 K.100—1100 K温度下拉应力随时间的变化
Relationship of peak pressure and temperature.拉应力峰值随温度的变化
Void volume fraction as a function of time at 100– 1100 K.100—1100 K温度下孔洞体积分数随时间的变化
Void nucleation time at 100–1100 K.100—1100 K温度下孔洞成核时间
Distribution of voids at 100–1100 K (void volume fraction is 0.1).100—1100 K温度下内部孔洞分布(孔洞体积分数为0.1时)
Void volume fraction as a function of time at 100−700 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下孔洞体积分数与拉应力的关系 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
Void distribution on the second-peak of tensile stress at 100−700 K.100−700 K温度下拉应力时程曲线第二峰值点孔洞分布
Evolution of dislocation density as a function of time at 100−1100 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下位错密度变化情况 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
Radial distribution function of the system at 100−1100 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下径向分布函数变化情况 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
Snapshots for the structural changes at 100−1100 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下内部结构变化 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
Crystal structure fraction as a function of time at 100−1100 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下内部晶体结构占比 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
Structural changes at different time at 300 K.300 K温度下系统内部结构变化
Bond energy of iron at 300−1100 K.300−1100 K温度下铁原子键能
Potential energy of the system at 100−1100 K.100−1100 K温度下系统势能
Comparison of void volume fraction between the NAG model and MD at 100−1100 K: (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K.100−1100 K温度下NAG与MD的孔洞体积分数结果的对比 (a) 100 K; (b) 300 K; (c) 500 K; (d) 700 K; (e) 900 K; (f) 1100 K
  • Table 1.

    Four characteristic points time at 100– 700 K.

    100—700 K温度下四个特征点时间

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    Table 1.

    Four characteristic points time at 100– 700 K.

    100—700 K温度下四个特征点时间

    温度/K时间/ps
    ABCD
    10015.716.517.519.1
    30013.414.515.417.9
    50012.613.814.917.7
    70013.113.914.617.6
  • Table 2.

    Best-fit NAG parameters at 100−1100 K.

    100−1100 K温度下NAG模型最佳拟合参数

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    Table 2.

    Best-fit NAG parameters at 100−1100 K.

    100−1100 K温度下NAG模型最佳拟合参数

    Pn0/Pa P1/Pa ${\dot N_0}$/m–3·s–1Pg0/Pa η/Pa·s Rn/m Σ
    100 K1.61 × 10101.42 × 1077.10 × 10152.75 × 1091.72 × 10–13.1 × 10–100.15
    300 K1.55 × 10102.35 × 1071.22 × 10152.48 × 1092.20 × 10–13.1 × 10–100.18
    500 K1.51 × 10101.18 × 1075.91 × 10142.15 × 1091.83 × 10–13.1 × 10–100.14
    700 K1.50 × 10103.31 × 1071.37 × 10162.02 × 1092.17 × 10–13.1 × 10–100.17
    900 K1.46 × 10102.76 × 1073.29 × 10151.98 × 1092.53 × 10–13.1 × 10–100.12
    1100 K1.33 × 10101.87 × 1071.88 × 10141.95 × 1092.11 × 10–13.1 × 10–100.17
    低碳钢[54]1.12 × 1091.0 × 1082.5 × 10142.0 × 1082.778 × 1023.0 × 10–5
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Yun-Tian Wang, Xiang-Guo Zeng, Xin Yang. Molecular dynamics simulation of effect of temperature on void nucleation and growth of single crystal iron at a high strain rate[J]. Acta Physica Sinica, 2019, 68(24): 246102-1

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Paper Information

Received: Jun. 14, 2019

Accepted: --

Published Online: Sep. 17, 2020

The Author Email:

DOI:10.7498/aps.68.20190920

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