Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/90766
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dc.contributorDepartment of Civil and Environmental Engineering-
dc.creatorShen, Cen_US
dc.creatorDeng, Xen_US
dc.creatorWei, Zen_US
dc.creatorDollevoet, Ren_US
dc.creatorZoeteman, Aen_US
dc.creatorLi, Zen_US
dc.date.accessioned2021-09-03T02:33:42Z-
dc.date.available2021-09-03T02:33:42Z-
dc.identifier.issn0020-7403en_US
dc.identifier.urihttp://hdl.handle.net/10397/90766-
dc.language.isoenen_US
dc.publisherPergamon Pressen_US
dc.rights© 2021 The Authors. Published by Elsevier Ltd. This is an open access article under the CC BY license ( http://creativecommons.org/licenses/by/4.0/)en_US
dc.rightsThe following publication Shen, C., Deng, X., Wei, Z., Dollevoet, R., Zoeteman, A., & Li, Z. (2021). Comparisons between beam and continuum models for modelling wheel-rail impact at a singular rail surface defect. International Journal of Mechanical Sciences, 198, 106400 is available at https://doi.org/10.1016/j.ijmecsci.2021.106400en_US
dc.subject3D solid finite elementen_US
dc.subjectImpact forceen_US
dc.subjectRail surface defecten_US
dc.subjectTimoshenko beamen_US
dc.subjectWave propagationen_US
dc.subjectWheel-rail contacten_US
dc.titleComparisons between beam and continuum models for modelling wheel-rail impact at a singular rail surface defecten_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.volume198en_US
dc.identifier.doi10.1016/j.ijmecsci.2021.106400en_US
dcterms.abstractA singular rail or wheel surface irregularity, such as a squat, insulation joint or wheel flat, can cause large wheel-rail impact force. Both the magnitude and frequency content of the impact force need to be correctly modelled because they are closely related to the formation, deterioration and detection of such irregularities. In this paper, we compare two types of commonly used wheel-track interaction models for wheel-rail impact problems, i.e., a beam and a continuum finite element model. We first reveal the differences between the impact forces predicted by the two models due to a typical rail squat using a time-frequency analysis. Subsequently, we identify the causes for the differences by evaluating the effects of different model assumptions, as well as different model parameters. Results show that the impact force consists of a forced vibration peak M1 followed by free vibration related oscillations with three dominant frequencies: f1 (340 Hz), f2 (890 Hz) and f3 (1120 Hz). Compared with the continuum model, the beam model with a Hertzian contact spring overestimates the M1 peak force. The discrepancy can be reduced by using a Winkler bedding contact model. For the track model, the beam model is comparable to the continuum model up to about 800 Hz, beyond which the track damping starts to deviate. As a result, above 500 Hz, the contact forces dominate at f2 for the beam while at f3 for the continuum model. Finally, we show that the continuum model is more accurate than the beam model by comparing to field observations. The effects of stress wave propagation on the differences are also discussed.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationInternational journal of mechanical sciences, 15 May 2021, v. 198, 106400en_US
dcterms.isPartOfInternational journal of mechanical sciencesen_US
dcterms.issued2021-05-
dc.identifier.scopus2-s2.0-85103414470-
dc.identifier.eissn1879-2162en_US
dc.identifier.artn106400en_US
dc.description.validate202109 bcvc-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumberOA_Scopus/WOS-
dc.description.pubStatusPublisheden_US
dc.description.oaCategoryCCen_US
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