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含椭圆孔有限大二十面体准晶板平面弹性问题的边界元分析

王会苹 王桂霞 陈德财

王会苹, 王桂霞, 陈德财. 含椭圆孔有限大二十面体准晶板平面弹性问题的边界元分析[J]. 应用数学和力学, 2024, 45(4): 400-415. doi: 10.21656/1000-0887.440241
引用本文: 王会苹, 王桂霞, 陈德财. 含椭圆孔有限大二十面体准晶板平面弹性问题的边界元分析[J]. 应用数学和力学, 2024, 45(4): 400-415. doi: 10.21656/1000-0887.440241
WANG Huiping, WANG Guixia, CHEN Decai. Boundary Element Analysis for the Plane Elasticity Problems of Finite Icosahedral Quasicrystal Plates Containing Elliptical Holes[J]. Applied Mathematics and Mechanics, 2024, 45(4): 400-415. doi: 10.21656/1000-0887.440241
Citation: WANG Huiping, WANG Guixia, CHEN Decai. Boundary Element Analysis for the Plane Elasticity Problems of Finite Icosahedral Quasicrystal Plates Containing Elliptical Holes[J]. Applied Mathematics and Mechanics, 2024, 45(4): 400-415. doi: 10.21656/1000-0887.440241

含椭圆孔有限大二十面体准晶板平面弹性问题的边界元分析

doi: 10.21656/1000-0887.440241
基金项目: 

国家自然科学基金 11962026

内蒙古自治区自然科学基金重点项目 2022ZD05

内蒙古自治区高校科研项目 NJZZ21003

详细信息
    作者简介:

    王会苹(1999—), 女, 硕士生(E-mail: whp7464@163.com)

    通讯作者:

    王桂霞(1968—), 女, 教授, 博士(通讯作者. E-mail: nsdwgx@126.com)

  • 中图分类号: O343.1;O343.4;O241.82

Boundary Element Analysis for the Plane Elasticity Problems of Finite Icosahedral Quasicrystal Plates Containing Elliptical Holes

  • 摘要: 基于扩展的Stroh方法, 对含椭圆孔有限大二十面体准晶板平面弹性问题进行边界元分析.首先利用扩展的Stroh方法, 研究了二十面体准晶的Green函数, 得到了含椭圆孔无限大二十面体准晶平面弹性问题位移和应力的基本解.利用该基本解, 通过加权余量法建立了区域内积分方程和边界积分方程, 并采用线性插值函数及Gauss积分对含未知量的边界积分方程和区域内积分方程分别进行离散,得到了离散格式.进一步, 对椭圆孔的孔边应力进行了数值求解, 并将有限大板的数值结果与无限大板的解析解进行了对比验证, 说明当板与椭圆孔尺寸之比小于某下限值时, 不能用无限大板的解析解对有限大板进行分析.最后, 分析了在垂向拉伸作用下, 板的大小、孔口尺寸及倾斜角度对孔边应力的影响.结果表明: 板的尺寸沿垂直拉伸方向变化对孔边应力的影响更明显; 随着椭圆孔尺寸的增加, 孔边应力集中现象越明显; 若长轴垂直拉伸方向, 椭圆孔倾斜会减缓孔边应力集中程度.
  • 图  1  构型及受力情况

    Figure  1.  The configuration and the force

    图  2  含椭圆孔的试样

    Figure  2.  The specimen containing an elliptical hole

    图  3  声子场应力集中系数随板尺寸的变化

    Figure  3.  The variations of phonon stress concentration coefficients with plate sizes

    图  4  边界元解与无限大板解析解对比(H/a=200, W/a=100)

    Figure  4.  Comparison of the boundary element solution and the infinite plate analytical solution(H/a=200, W/a=100)

    图  5  边界元解与无限大板解析解对比(H/a=40, W/a=8)

    Figure  5.  Comparison of the boundary element solution and the infinite plate analytical solution (H/a=40, W/a=8)

    图  6  a=0.2 m,孔边应力值随b的变化情况

    Figure  6.  For a=0.2 m, the changes of hole edge stresses with b

    图  7  b=0.1 m,孔边应力值随a的变化情况

    Figure  7.  For b=0.1 m, the changes of hole edge stresses with a

    图  8  椭圆孔旋转构型

    Figure  8.  The configuration diagram of the elliptic hole rotation

    图  9  椭圆孔边应力随α的变化情况

    Figure  9.  The changes of hole edge stresses with α

    图  10  应力强度因子随2a/W的变化情况

    Figure  10.  The variation of stress intensity factor with 2a/W

    表  1  应力集中系数随α的变化情况

    Table  1.   The change of the stress concentration coefficient with α

    α/(°)
    0 15 45 75 90
    stress concentration coefficient 5.098 2 4.767 9 3.651 6 2.258 2 2.018 6
    下载: 导出CSV
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  • 收稿日期:  2023-08-14
  • 修回日期:  2023-12-12
  • 刊出日期:  2024-04-01

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