吉林大学学报(工学版) ›› 2026, Vol. 56 ›› Issue (3): 758-771.doi: 10.13229/j.cnki.jdxbgxb.20240914

• 交通运输工程·土木工程 • 上一篇    

沥青路面轴对称动力响应问题中解析解对比

尚桦雨1,2(),范海山1,2,张军辉1,2()   

  1. 1.长沙理工大学 公路工程教育部重点实验室,长沙 410114
    2.长沙理工大学 交通学院,长沙 410114
  • 收稿日期:2024-08-19 出版日期:2026-03-01 发布日期:2026-03-31
  • 通讯作者: 张军辉 E-mail:shy@stu.csust.edu.cn;zjhseu@csust.edu.cn
  • 作者简介:尚桦雨(1999-),男,博士研究生.研究方向:耐久性路基设计理论与方法.E-mail:shy@stu.csust.edu.cn
  • 基金资助:
    国家自然科学基金项目(52025085);国家自然科学基金项目(52338009)

Comparative of analytical solutions for axial symmetric dynamic response of asphalt pavements

Hua-yu SHANG1,2(),Hai-shan FAN1,2,Jun-hui ZHANG1,2()   

  1. 1.Key Laboratory for Highway Engineering of Ministry of Education,Changsha University of Science and Technology,Changsha 410114,China
    2.School of Transportation,Changsha University of Science& Technology,Changsha 410114,China
  • Received:2024-08-19 Online:2026-03-01 Published:2026-03-31
  • Contact: Jun-hui ZHANG E-mail:shy@stu.csust.edu.cn;zjhseu@csust.edu.cn

摘要:

当前有关路面力学的研究多集中于解析解推导以及影响因素探究上,缺乏不同解析解方法的差异性研究。为此,本文分别以传递矩阵法、刚度矩阵法、波传递法以及反射、透射矩阵法推导出了考虑材料横观各向同性以及层间接触状态的轴对称路面结构动力响应解析解。在此基础上,结合4种路面结构研究了上述4种解析解的计算效率以及适用范围。结果表明:①在矩阵规模上,由小到大依次为反射、透射矩阵法、传递矩阵法、刚度矩阵法以及波传递法;②在求解速度上,传递矩阵法耗时显著少于其余3种解析解方法,且反射、透射矩阵法耗时最长;③在数值稳定性上,传递矩阵法在进行有限厚度的动力响应计算时极易出现数值溢出问题,而其余解析解方法均具有较好的数值稳定性;④在实际应用上,传递矩阵法尤其适用于求解半空间体表面弯沉;刚度矩阵法仅可计算各结构层表面的动力响应;而波传递法和反射、透射矩阵法可求解路面内部任意位置的动力响应。

关键词: 层状体系力学, 传递矩阵, 刚度矩阵, 波传递, 反射、透射矩阵

Abstract:

The current researches on pavement mechanics usually focus on the derivation of analytical solutions and the exploration of the factors affecting them, there are few studies on the difference of analytical solutions. In order to solve this problem, transfer matrix method, stiffness matrix method, wave transfer method and reflection and transmission matrix method were applied in the deduction process of the analytical solutions considering the transverse isotropy of materials and the contact state between layers. On this basis, the calculation efficiency and the range of adaptability of the above four analytical solutions are studied by combining four kinds of pavement structures. The results show that: ①for the matrix scale, reflection and transmission matrix method, transfer matrix method, stiffness matrix method and wave transfer method increase in turn; ② for the solution speed, the transfer matrix method takes much less time than the other three methods, while the reflection and transmission matrix method consumes the most time; ③in the numerical stability, the transfer matrix method is very easy to overflow data when calculating the dynamic response of finite thickness, while the other analytical solution methods have good numerical stability; ④in practical application, the transfer matrix method is particularly suitable for the surface of semi space problems, and the stiffness matrix method can only calculate the dynamic response of the surface of each structural layer, however, the wave transfer method and the reflection and transmission matrix method can solve the dynamic response of any position in the pavement.

Key words: mechanics of the layered system, transfer matrix method, stiffness matrix method, wave transfer method, reflection and transmission matrix method

中图分类号: 

  • U416.2

图1

N层层状体系示意图"

表1

路面结构层材料参数"

结构层Ev/MPanμv(=μhρ/(kg?m-3h/mαx
路面7 0000.30.252 4000.180.8
基层10 0000.50.302 3000.350.0
底基层4001.00.352 2000.200.0
土基1001.00.351 6003.00-

图2

不同解析解计算结果对比 (χ=300, ΔL=5)"

图3

弯沉曲线收敛探究 (刚度矩阵法)"

图4

水平应变曲线收敛探究 (刚度矩阵法)"

图5

弯沉峰值收敛探究 (刚度矩阵法)"

图6

文献对比"

图7

路面结构示意图"

表2

不同求解方法计算耗时 (s)"

计算方法路面结构传递/反射透射矩阵/矩阵元素计算构建矩阵方程并求解数值逆变换总耗时

传递矩

阵法

A76.354.428.9160.9
B计算失败,计算结果为NAN
C80.254.728.9191.1
D计算失败,计算结果为NAN

刚度矩

阵法

A423.4121.330.2590.7
B398.2116.827.9557.3
C554.4141.430.1741.5
D531.5138.627.8712.8

波传

递法

A123.2396.631.0643.1
B113.5401.828.2629.1
C158.4496.429.7821.7
D147.7499.728.0803.9

反射、

透射

矩阵法

A76.8555.130.5677.8
B70.4559.229.1674.3
C101.3745.431.6894.1
D95.5756.129.1895.8

图8

不同路面结构表面弯沉"

表3

不同解析解特点及适用范围"

计算方法

计算

速度

数值

稳定性

求解位置适应范围
传递矩阵法较稳定路面表面半空间
刚度矩阵法一般稳定各结构层表面

半空间

有限厚度

波传递法较慢稳定任意位置

半空间

有限厚度

反射、透射矩阵法较慢稳定任意位置

半空间

有限厚度

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