Dynamic Axle Loads on Tracks with and Without Ballast Mats: Numerical Results of Three-Dimensional Vehicle-Track-Soil Models

Abstract Ballast mats are an efficient measure to reduce the vibrations near railway lines. The vehicle-track system gets a low eigenfrequency due to the insertion of an elastic ballast mat under the ballast. For frequencies higher than this low vehicle-track eigenfrequency, the forces, which are generating the vibration of the soil, are considerably reduced. In this contribution, a combined finite-element boundary-matrix method is used to calculate a number of completely three-dimensional track models with and without ballast mats. The influence of the important parameters such as the stiffness of the ballast mat, the unsprung vehicle mass, the mass of the track, and the stiffness of the subsoil is investigated. The numerical results are presented as the transfer functions of the total force that is acting on the soil and generating the vibration of the environment. The effectiveness of ballast mats is achieved by division of two of these force functions. The general tendencies for this insertion loss are discussed and a comparison with measurements is given. To come to an improved practical tool for the design of ballast-mat tracks, the finite-element method results are approximated by a simple two-dimensional model of which the solution is given explicitly.

[1]  Lars Vabbersgaard Andersen,et al.  Vibration from a railway tunnel predicted by coupled finite element and boundary element analysis in two and three dimensions , 2002 .

[2]  C. E. Hanson,et al.  Performance of ballast mats on passenger railroads: Measurement vs. projections , 2006 .

[3]  R. Wettschureck,et al.  Geräusche und Erschütterungen dem Schienenverkehr , 2004 .

[4]  Lutz Auersch,et al.  The excitation of ground vibration by rail traffic: theory of vehicle–track–soil interaction and measurements on high-speed lines , 2005 .

[5]  Lutz Auersch,et al.  Praxisgerechtees Prognosemodell für Erschütterungen: Einfache Rechenverfahren für die Emission, Transmission und Immission , 2003 .

[6]  Francisco J. Sánchez-Sesma,et al.  Seismic response of three-dimensional alluvial valleys for incident P, S, and Rayleigh waves , 1995 .

[7]  L. Auersch,et al.  Das Fahrzeug-Fahrweg-Verhalten und die Umgebungserschuetterungen bei Eisenbahnen , 2001 .

[8]  Ulrich Moehler,et al.  Effectiveness of vibration preventive measures with consideration of modified properties of trainsets , 2004 .

[9]  Chris Jones,et al.  Prediction of ground vibration from trains using the wavenumber finite and boundary element methods , 2006 .

[10]  F. H. Müller-Boruttau,et al.  Dynamische Fahrbahnmodelle für HGV-Strecken und Folgerungen für Komponenten , 1998 .

[11]  L. Auersch,et al.  A simple boundary element formulation and its application to wavefield excited soil‐structure interaction , 1990 .

[12]  Jens Dinkel Ein semi-analytisches Modell zur dynamischen Berechnung des gekoppelten Systems Fahrzeug-Fahrweg-Untergrund für das Oberbausystem Feste Fahrbahn , 2000 .

[13]  Lutz Auersch,et al.  Wave propagation in layered soils : theoretical solution in wavenumber domain and experimental results of hammer and railway traffic excitation , 1994 .

[14]  L Girardi PROPAGATION DES VIBRATIONS DANS LES SOLS HOMOGENES OU STRATIFIES , 1981 .

[15]  Klaus Knothe,et al.  Receptance behaviour of railway track and subgrade , 1998 .

[16]  Werner Rücker Dynamic interaction of a railroad-bed with the subsoil , 1982 .