移动荷载对不间断圆柱形隧道的作用

I. S. Ismail, N. Kuldashov, Nuriddinov
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引用次数: 0

摘要

本文介绍了考虑地表影响的隧道、管道等地下长输运结构移动荷载作用的计算技术基础。在弹性模型上,考虑了不同层理深度下未加筋和加筋结构的动力特性,以及运行荷载类型和参数对岩体应力-应变状态的影响。货物的运动速度被认为是亚音速的,这与被调查的地下物体的现代运输速度相对应。为了描述半空间厚壁壳的运动,采用了位移势弹性理论的动力学方程,而对于薄壁壳,则采用了经典的薄壳理论方程。方程在与载荷相关的运动坐标系中书写。构造了一个封闭的微分方程组。微分方程组用分离变量法、傅里叶积分变换、Romberg、Muller和Gauss法求解。通过对数值结果的分析可知,在这些情况下,隧道的加固使地表移动荷载的动力效应减小。在移动荷载作用下,地表对岩体应力-应变状态的影响是不均匀的。对于周期较短的负载,这种影响几乎不明显,并且在非常小的周期内变得明显。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the action of mobile loads on an uninterrupted cylindrical tunnel
He article gives the basics of the calculation technique for the action of mobile loads of long underground transport structures such as tunnels and pipelines taking into account the influence of the earth's surface. On elastic models, the dynamic behavior of unreinforced and reinforced structures at different depths of bedding is considered, as well as the effect of the type and parameters of the running load on the stress-strain state of the rock massif. The speed of the movement of the cargo is considered subsonic, which corresponds to the modern speeds of transport in the investigated underground objects. To describe the motion of a half-space and thick-walled shells, dynamic equations of the theory of elasticity in displacement potentials are used, and for thin-walled shells the classical equations of the theory of thin shells are used. Equations are written in a moving coordinate system associated with the load. A closed system of differential equations is constructed. The system of differential equations is solved by the method of separated variables, integral Fourier transforms, the Romberg, Muller and Gauss method. From the analysis of the obtained numerical results it follows that in these cases the reinforcement of the tunnel leads to a decrease in the dynamic effect of the moving loads on the earth's surface. The Earth's surface has an uneven effect on the stress-strain state of the rock massif under the action of moving loads. For a load with a shorter period, this effect is almost not noticeable, and becomes noticeable for very small periods.
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