Letter to the EditorDynamic response analyses of vehicle and track coupled system on track transition of conventional high speed railway
Introduction
Transition regions are locations where a railway track exhibits abrupt changes in vertical stiffness [1]. They usually occur at the abutments of open deck bridges, where a concrete sleeper track changes to a wooden sleeper track, at the ends of a tunnel, at highway level crossings, at locations where rigid culverts are placed close to the bottom of the sleepers in a ballasted track, etc., shown in Fig. 1. Track transitions caused by a change of rail cross-section are rare and their effect is generally very small. Therefore, they will not be considered here.
Transition regions require frequent maintenance. When neglected, they will deteriorate at an accelerated rate. This may lead to pumping ballast, swinging or hanging sleepers, permanent rail deformations, worn track components, and loss of surface and gauge. These in turn may create a potential for a derailment.
A large quantity of abutments of open deck bridges, road crossings and tunnel ends exist in Chinese railway lines. For instance, the total length of the Beijing-Shanghai railway line is 1459 km and there are 1471 abutments of bridges and 490 road crossings on this line. In the past, the average speed of the trains in China usually was less than 80 km/h. The track transition problem is not serious in this situation. However, it has to be solved as the speed of trains in China is increased. The maximum train speed possible is 160 km/h according to Chinese railway regulation [2].
To clarify this problem, a dynamic computational model for the vehicle and track coupled system is developed by means of the finite element method. In numerical implementation, the vehicle and the track coupled system is divided into two parts, i.e., lower structure and upper structure. The vehicle as upper structure in the coupled system is a whole locomotive or carriage with two layers of springs and dampers in which vertical and pitch motion for the vehicle body and bogie are included. The lower structure in the coupled system is railway track where rails are considered as beams with finite length resting on a double layer continuous elastic foundation. The two parts are solved independently with an iterative scheme. Coupling the vehicle system and the railway track is realized through interaction forces between the wheels and the rail. Based on the model, dynamic response analyses of the vehicle and track coupled system at a track transition are then performed, where various train speeds and different settlements on track transitions are considered, and some conclusions are given.
Section snippets
Models for analysis of the vehicle and track coupled system
Studies [3], [4], [5], [6], [7], [8], [9], [10], [11], [12], [13], [14] have been published on the vibration in a railway track under moving vehicles and different theories and models have been presented. In this paper, a more comprehensive dynamic analysis model for the vehicle and track coupled system will be developed.
Since the vehicle and the railway track are symmetrical about the centreline of the track and the longitudinal motion of the track has no effect on results, only half of the
Numerical algorithms
In the numerical implementation, we will divide the vehicle and track coupled system into two parts, lower structure and upper structure, and solve them independently with an iterative scheme [13], [14], [16], [20], [21]. Coupling the vehicle system and the railway track can be realized through interaction forces between wheels and rail. The track vertical profile irregularity will be considered in calculating the interaction forces with the conventional Hertz formula. One advantage is that we
Verification
In order to test the effectiveness and the correctness of the model, the dynamic interaction forces between one wheel and the rail at a joint are analyzed, where 1.5 mm unevenness of level at the joint and different train speeds are considered. The parameters for the computation [18] are as follows:
C62 Chinese carriage with 210 kN axle load, Cs1=0, ,
, ,
rail cross-section area: , moment of inertia: ,
modules of elasticity:
Dynamic response analyses of vehicle and track coupled system on track transition
In the analyses of dynamic responses on the track transition, a TGV (French high speed train) locomotive is considered in this paper, as shown in Fig. 5. Parameters for the TGV locomotive are given in Table 2. In order to reduce the boundary effects of the rail, the total track length for the computation is 230.85 m (20 m for the transition region) with 405 generalized beam elements, which is more than 10 times the length of the vehicle. The running distance for the vehicle is 180 m. The track
Conclusions
The amplitudes of vibration and the corresponding accelerations generated in the vehicle and the rail and the interaction forces between the vehicle and the rail in a track transition due to different irregularity angles of the track and at various train speeds have been analyzed here numerically by a vehicle and track coupled computational model. The vehicle as upper structure in the coupled system is a whole locomotive or carriage with two layers of springs and dampers in which the vertical
Acknowledgements
The work reported herein was supported by Natural Science Foundation of China (50268001) and Natural Science Foundation of Jiangxi Province (0250034).
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