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J4  2014, Vol. 48 Issue (2): 228-235    DOI: 10.3785/j.issn.1008-973X.2014.02.007
    
Time step length determination of Newmark method for dynamic responses of railway tracks
SHI Li1, CAI Yuan-qiang1,2, XU Chang-jie1
1.Key Laboratory of Soft Soils and Geoenvironmental Engineering of Ministry of Education, Zhejiang University,
Hangzhou 310027; 2.College of Architecture and Civil Engineering, Wenzhou University, Wenzhou 325035
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Abstract  

To determine the time step length in calculating dynamic responses of railway tracks by using the Newmark method, a track model consisting of a rail beam on two layers of discrete supports was studied analytically to obtain the amplitude spectrums of the rail-sleeper dynamic reaction forces for a single point load moving at different velocities. Subsequently, the track model was discretized spatially by mode superposition method and the temporal solutions of the resulting equations were obtained by the Newmark method using different time step length. By comparing the temporal results with those obtained by the highly accurate Runge-Kutta integration method, it is found that the time step length of the Newmark method should satisfy the Nyquist theorem. And the frequency band in the Nyquist theorem should be wide enough to include at least the first two valleys of the amplitude spectrum of the rail-sleeper dynamic interaction force, which are contributed by the moving load periodically passing through the discrete supports. As an example, a track model consisting of a rail beam on three layers of discrete supports was studied to obtain the sleeper and the ballast accelerations by the Newmark method with the time step length being determined by the Nyquist theorem.



Published: 01 February 2014
CLC:  TU 45  
Cite this article:

SHI Li, CAI Yuan-qiang, XU Chang-jie. Time step length determination of Newmark method for dynamic responses of railway tracks. J4, 2014, 48(2): 228-235.

URL:

http://www.zjujournals.com/eng/10.3785/j.issn.1008-973X.2014.02.007     OR     http://www.zjujournals.com/eng/Y2014/V48/I2/228


轨道结构动力响应Newmark方法时间积分步长的确定

为了明确轨道结构动力响应计算中Newmark方法时间积分步长的确定依据,采用双层离散点支承轨道结构模型解析求解不同移动速度点荷载作用下的轨枕动反力频谱,进而采用模态叠加法和Newmark方法求解不同时间积分步长下上述双层轨道结构的位移和加速度响应,并与高精度的四阶Runge-Kutta方法计算结果对比.结果表明,不同荷载移动速度下的时间积分步长均应满足Nyquist采样定理,且采样定理中的频带宽度应至少包括由离散支承参数激励引起的轨枕动反力频谱的前二阶谷值.作为算例,根据上述采样定理确定的时间积分步长,采用Newmark方法计算了移动列车轴荷载作用下三层离散点支承轨道的枕木及道砟加速度响应.

[1] MEIROVITCH L. Analysis method in vibrations [M]. London: MacMillan, 1967: 102-105.
[2] XU Y L, LI Q, WU D J, et al. Stress and acceleration analysis of coupled vehicle and long-span bridge systems using the mode superposition method [J]. Engineering Structures, 2010, 32: 1356-1368.
[3] RIEKER J R, LIN Y H, TRETHEWEY M W. Discretization conderations in moving load finite element beam models [J]. Finite Elements in Analysis and Design, 1996, 21: 129-144.
[4] OLSSON M. On the fundamental moving load problem [J]. Journal of Sound and Vibration, 1991, 145(2): 299-307.
[5] WU J J, WHITTAKER A R, CARTMELL M P. The use of finite element techniques for calculating the dynamic response of structures to moving loads [J]. Computers & Strucuters, 2000, 78: 789-799.
[6] LIN Y H, TRETHWEY M W. Finite element analysis of elastic beams subjected to moving dynamic load [J]. Journal of Sound and Vibration, 1990, 136(2): 323342.
[7] HENCHI K, FAFARD M, TALBOT M, et al. An efficient algorithm for dynamic analysis of bridges under moving vehicles using a coupled modal and physical components approach [J]. Journal of Sound and Vibration, 1998, 212(4): 663-683.
[8] THAMBIRATNAM D, ZHUGE Y. Dynamic analysis of beams on an elastic foundation subjected to moving loads [J]. Journal of Sound and Vibration, 1996, 198(2): 149-169.
[9] JU S H, LIN H T, HSUEH C C, et al. A simple finite element model for vibration analysis induced by moving vehicles [J]. International Journal for Numerical Methods in Engineering, 2006, 68: 1232-1256.
[10] JAFARI A A, EFTEKHARI S A. A new mixed finite element differential quadrature formulation for forced vibration of beams carrying moving loads [J]. Journal of Applied Mechanics, 2011, 78: 1-16.
[11] 李有法.数值计算方法[M].北京:高等教育出版社,1996: 56-58.
[12] 翟婉明.车辆-轨道耦合动力学[M].3版.北京:科学出版社,2007: 72-75.
[13] ZHAI W M, WANG K Y, LIN J H. Modeling and experiment of railway ballast vibrations [J]. Journal of Sound and Vibration, 2004, 270: 673-683.
[14] 蔡袁强,王玉,曹志刚,等.列车运行时由轨道不平顺引起的地基振动研究[J].岩土力学,2012, 33(2): 327-335.
CAI Yuan-qiang, WANG Yu, CAO Zhi-gang, et al. Study of ground vibration from trains caused by track irregularities [J]. Rock and Soil Mechanics, 2012, 33(2): 327-335.
[15] TAKEMIYA H, BIAN X C. Substructure simulation of inhomogeneous track and layered ground dynamic interaction under train passage [J]. Journal of Engineering Mechanics, 2005, 131: 699-711.
[16] AUERSCH L. The excitation of ground vibration by rail traffic: theory of vehicle-track-soil interaction and measurements on high-speed lines [J]. Journal of Sound and Vibration, 2005, 284: 103-132.

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