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Civil-Comp Proceedings
ISSN 1759-3433 CCP: 104
PROCEEDINGS OF THE SECOND INTERNATIONAL CONFERENCE ON RAILWAY TECHNOLOGY: RESEARCH, DEVELOPMENT AND MAINTENANCE Edited by: J. Pombo
Paper 133
Spectral Analysis of Train-Related Dynamic Loads Acting on a Ballast Layer A. Aikawa and H. Sakai
Railway Technical Research Institute, Tokyo, Japan A. Aikawa, H. Sakai, "Spectral Analysis of Train-Related Dynamic Loads Acting on a Ballast Layer", in J. Pombo, (Editor), "Proceedings of the Second International Conference on Railway Technology: Research, Development and Maintenance", Civil-Comp Press, Stirlingshire, UK, Paper 133, 2014. doi:10.4203/ccp.104.133
Keywords: ballasted track, spectral analysis, field measurement, finite element method, elastic vibration mode, rigid-body vibration mode.
Summary
Spectral analysis, based on train-related dynamic loads acting on an existing ballast
layer which were directly measured at 10 kHz sampling intervals, revealed that
dynamic response loads acting on a ballast layer consist of vibration components
with a very wide frequency range. The accelerating curve regarding ballast dynamic
response indicated that the first-order elastic resonance mode of the ballast aggregate
around 650-700Hz in which the whole ballast aggregate repeats the vertical
expansion and shrinkage elastically. Finite Element transient response analysis using
the ballast aggregate model revealed that the natural frequency of the first-order
natural mode which represents the vertical motion of the entire aggregate is around
730Hz in the case of a 40cm thick ballast layer. This analytical result coincides
substantially with the measured one. The compliance curve identified the rigid body
vibrational mode at around 40Hz at which a mass of the track structure with an
additional mass given by a train vibrates simultaneously up and down as a result of
the spring stiffness of the ballast layer. A weak roadbed and excessive overburden
mass theoretically cause the reduction of the frequency in the rigid body mode.
Therefore, it can be inferred that the occurrence of ballast resonance with the
passing-axle frequency causes the shift and the flow of ballast gravel.
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