Time domain 3D finite element modelling of train-induced vibration at high speed
Introduction
During the past decades, important developments have taken place to provide guidance on a safe and cost effective design for constructing high speed trains. This is driven by the increase in the train speed, axle loads and the construction of new high speed lines, and their resulting vibration effects on the track and nearby buildings due to the waves transmitted through the soil. In soft ground sites, high levels of vibration can be produced, when the train speed exceeds the ground Rayleigh wave speed. Understanding the related wave propagation problems becomes necessary, when looking at mitigation strategies, to allow the safe and reliable operation of high-speed trains over poor ground.
Various models have been developed to predict the generation and propagation of ground vibration due to train passage. Most of the early works are based on analytical or semi-analytical approaches and deal with moving point load induced ground vibration (see Refs. [1], [2], [3], [4], [5], [6], [7], [8], [9], e.g.). Further related bibliography references can be found in [10] and [11]. With the rapid progress of computer technologies, models based on the finite element method, the boundary element method, or coupled together, become more suited for solving soil dynamic problems. The FE method can be used in problems with complex geometry. However, when dealing with infinite domains, absorbing boundary conditions may be implemented to avoid wave reflection.
The objective of the present work is to numerically enhance a 3D FE coupled train-track model which predicts the ground vibration of high speed train and heavy axle load conditions. References on advanced models incorporating the dynamic excitation are given in the research work of Galvín et al. [12], where a coupled finite element – boundary element model is used. This model incorporates the train-track interaction and solves non-linear coupled equations using an implicit time integration scheme. This involves assembling the global coupled system matrices, which requires large computational memory capacity.
The model proposed in this paper also takes into account the train-track interaction mechanisms and the sleeper-ballast interaction. It also accounts for the spread of the moving load on the adjacent sleepers via the rail and afterwards into the multi-layered subgrade. This model may deal with material nonlinearity, multi-layered ground and material damping. Moreover, this 3D FE model combines explicit time stepping with an element-by-element storage procedure and hence it does not require significant memory allocation and may be more suited for parallelization. The rail is represented by 3D Euler–Bernoulli beam elements. A multi degrees of freedom vehicle dynamic model [13] is incorporated and coupled to the 3D track model, based on the non linear contact theory. The program can also look at ground vibration generated due to track irregularities, such as those from short or long wavelength track faults, or from irregularities on the rail surface.
The structure of this paper is as follows. The next section details the presentation of the numerical model. This includes a brief description of the vehicle dynamic model, the material damping approach, the finite elements used in the approximation of the track model and the adopted explicit time integration scheme. Validation results based on the analytical solution of the Boussinesq’s problem, where a homogeneous half space is subjected to a static constant point load, are presented. Finally, numerical tests are performed to study the influence of the train’s fundamental passing frequency for different train speeds including the subcritical and supercritical ranges. The effect of material damping model is also presented.
Section snippets
The numerical model
The developed model involves the vehicle, the track and the ground. Since the loading is assumed to be symmetrically distributed on the two rails, half of the car body is sufficient to derive the train model. Only vertical vibrations are taken into account. In this paper, the vehicle dynamic is governed by a quarter train model consisting of a car body, bogies and suspension systems [13]. The latter is coupled with the three dimensional track model by virtue of the non linear contact theory.
Numerical results
Various numerical experiments are carried out using the proposed 3D FE coupled train-track model in order to investigate the performance of the material damping approach considered in this work and the effect of the train speed on the dynamic response of the railway track. The 3D FE model was validated against experimental results in [21]. Validation results against Boussinesq’s analytical solution are first presented in the next subsection.
The train parameters used in this work are illustrated
Conclusion
A three dimensional finite element coupled train-track model incorporating train-track dynamic interaction and material damping is numerically studied in order to predict the track vibration at high train speeds, especially when it exceeds the Rayleigh ground speed. The influence of the material damping on the track responses are illustrated through different numerical tests. The attenuation effect in terms of the vertical response of the coupled train-track is clearly observed for higher train
Acknowledgement
The authors are grateful to the EPSRC for funding this work under Grant EP/H027262/1.
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