适用于铅锡合金动态响应的机器学习势函数

侯恩则 王啸洋 王涵

侯恩则, 王啸洋, 王涵. 适用于铅锡合金动态响应的机器学习势函数[J]. 高压物理学报. doi: 10.11858/gywlxb.20251151
引用本文: 侯恩则, 王啸洋, 王涵. 适用于铅锡合金动态响应的机器学习势函数[J]. 高压物理学报. doi: 10.11858/gywlxb.20251151
HOU Enze, WANG Xiaoyang, WANG Han. A Machine Learning Potential Model for Simulating Dynamic Mechanical Response of Pb-Sn Alloy[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20251151
Citation: HOU Enze, WANG Xiaoyang, WANG Han. A Machine Learning Potential Model for Simulating Dynamic Mechanical Response of Pb-Sn Alloy[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20251151

适用于铅锡合金动态响应的机器学习势函数

doi: 10.11858/gywlxb.20251151
详细信息
    作者简介:

    侯恩则(1999-),男,博士研究生,主要从事偏微分方程数值解、科学计算与机器学习研究. E-mail:sg.enzo.h@foxmail.com

    王啸洋(1991-),男,博士,助理研究员,主要从事材料辐照损伤、高压相结构预测、动态力学响应研究. E-mail:wang_xiaoyang@iapcm.ac.cn

  • 中图分类号: O521.2

A Machine Learning Potential Model for Simulating Dynamic Mechanical Response of Pb-Sn Alloy

  • 摘要: 铅是一种低熔点且具有复杂温度-压力相图的金属材料,经过与锡的合金化,能够进一步降低其熔点,使得铅锡合金成为研究材料动态力学响应及动态破坏行为的重要模型材料。目前,受表征手段的限制,通过实验方法揭示铅锡合金在原子尺度上的动态破坏行为和机理仍存在巨大挑战。非平衡分子动力学是一种重要的理论研究手段,可以模拟动态过程中的原子运动轨迹,从而揭示动态加载-卸载及破坏行为中的关键原子尺度过程。然而,分子动力学方法的可靠性依赖其所采用的原子间相互作用势函数的精度,目前并没有适用于铅锡合金的动态响应研究的高精度势函数,因此,制约了铅锡合金的动态模拟研究。通过同步学习策略,构建了压力为0~100 GPa、温度为0~5 000 K下具有第一性原理精度的铅锡合金机器学习势函数模型DP-PbSn。该势函数能够以第一性原理的精度预测铅锡合金的点阵常数和弹性常数等基本性质,以及表面能、层错能、空位形成能等缺陷性质,还能够准确地预测其熔化线和冲击Hugoniot曲线,展现了其在动态响应模拟过程中的适用性。利用该势函数对铅和铅锡合金的动态力学响应行为进行了初步的模拟研究,揭示了锡对动态加载过程中相变及塑性行为的影响。该势函数作为重要的理论工具,能够实现高精度的非平衡分子动力学模拟,从而为铅锡合金动态力学损伤行为的实验研究提供关键理论依据。

     

  • 图  不同温度、压力条件下3种组分的测试误差

    Figure  1.  Testing RMSE on three components at various temperature and pressure

    图  DP-PbSn沿着$ \langle 1\overline{1}0\rangle $方向滑移时不同滑移面上的广义层错能

    Figure  2.  Generalized stacking fault energy predicted by DP-PbSn along $ \langle 1\overline{1}0\rangle $ on various slip planes

    图  DP-PbSn及现有的EAM势函数[12]对0~100 GPa下的Pb熔点预测结果

    Figure  3.  Melting curves of Pb within the pressure range of 0–100 GPa predicted by DP-PbSn and EAM potential function[12]

    图  DP-PbSn预测的Hugoniot曲线

    Figure  4.  Hugoniot curves predicted by DP-PbSn

    图  不同速率下活塞冲击过程中体系的温度和压强分布

    Figure  5.  Distribution of pressure and temperature during dynamic loading at various velocities

    图  不同活塞速率下Pb和PbSn合金在加载过程中的分子动力学轨道截图(模拟时间为活塞加载后的20 ps)

    Figure  6.  NEMD snapshots for Pb and PbSn alloy at various piston velocities (snapshots were taken 20 ps after the piston loading)

    表  1  DP-PbSn的训练误差与测试误差

    Table  1.   Training and testing error of DP-PbSn

    Dataset RMSE
    Energy/(meV/atom) Force/(meV·Å–1) Virial stress/(meV/atom)
    Training 4.76 61.98 32.54
    Testing 2.88 31.39 25.73
    下载: 导出CSV

    表  2  利用DP-PbSn预测的纯Pb的基本性质

    Table  2.   Basic properties of pure Pb predicted by DP-PbSn

    Phase Model a Ecoh/eV C11/GPa C12/GPa C44/GPa Esurf/(meV·Å–2) Evac/eV
    (100) (110) (111)
    FCC DP-PbSn 5.037 –3.243 45.75 39.14 14.64 18.87 20.82 17.68 0.485
    DFT 5.039 –3.247 51.80 34.52 16.79 18.78 22.48 17.26 0.490
    Phase Model a c c/a Ecoh/eV C11/GPa C12/GPa C44/GPa Evac/eV
    HCP DP-PbSn 3.539 5.892 1.665 –3.238 58.032 38.603 5.162 0.530
    DFT 3.542 5.863 1.655 –3.234 51.840 35.560 6.950 0.520
    下载: 导出CSV

    表  3  利用DP-PbSn预测的不同组分PbSn合金的基本性质

    Table  3.   Basic properties of PbSn alloys with different compositions predicted by DP-PbSn

    Phase aSn/% Model a C11/GPa C12/GPa C44/GPa Esol/
    (meV/atom)
    Esurf/(meV·Å–2)
    (100) (110) (111)
    FCC 9 DP-PbSn 5.031 44.78 38.79 13.81 88.57 18.92 20.22 17.53
    DFT 5.021 51.28 35.19 14.25 127.09 20.10 22.40 19.20
    25 DP-PbSn 5.001 45.45 38.93 13.01 72.97 19.42 20.82 18.45
    DFT 4.991 51.21 36.28 12.53 95.39 22.60 24.60 23.90
    Phase aSn/% Model a c c/a C11/GPa C12/GPa C44/GPa Esol/
    (meV/atom)
    HCP 9 DP-PbSn 3.541 5.862 1.656 55.73 36.98 5.40 133.90
    DFT 3.541 5.846 1.651 55.26 40.71 11.29 252.10
    25 DP-PbSn 3.519 5.824 1.655 54.29 38.33 3.97 96.08
    DFT 3.465 5.885 1.698 55.71 40.34 5.16 157.06
    下载: 导出CSV
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出版历程
  • 收稿日期:  2025-08-06
  • 修回日期:  2025-10-27
  • 录用日期:  2025-11-28
  • 网络出版日期:  2025-10-29

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