
Mathematical model of the formation and development of wave-shaped rail wear when an electric locomotive operates in the traction mode in tangent sections of the track
Author(s) -
А. Я. Коган
Publication year - 2019
Publication title -
vestnik naučno-issledovatelʹskogo instituta železnodorožnogo transporta/vestnik naučno-issledovatelʹskogo instituta železnodorožnogo transporta
Language(s) - English
Resource type - Journals
eISSN - 2713-2560
pISSN - 2223-9731
DOI - 10.21780/2223-9731-2019-78-3-131-140
Subject(s) - traction (geology) , engineering , flange , electric locomotive , axle , tangent , bogie , track (disk drive) , traction motor , structural engineering , mechanics , mechanical engineering , physics , geometry , mathematics
The problem of wave-shaped rail wear is highly relevant for rail transport. The paper presents a mathematical model of the formation and development of wave-shaped rail wear. The task of estimating vertical wear of the rail head under the axles of electric locomotives passing in the traction mode is considered. A technique has been developed that allows building chain of calculations that determine the formation and development of a wave-shaped rail head wear. A specific calculation example is given, illustrating the process of propagation of a wave-shaped wear from the source of its formation in the direction of train motion. An example of the calculation allows drawing the following conclusions: 1. Wave-shaped wear primarily occurs when the shock interaction of the wheel of an electric locomotive moving in the traction mode and a rail thread having imperfections of the rolling surface. Such imperfections, among others, may be a joint with a significant gap or a “step down” in the direction of the locomotive, as well as a welded joint with defect 46.3-4. 2. Wavelength of the wave-shaped rail wear, its configuration and amplitude of the fundamental tone are determined mainly by joint oscillations of the wheel-motor unit of the locomotive and the track infrastructure in the field of high-frequency oscillations (120 – 180 Hz). 3. Multivariate calculations showed that in steady state, the distribution speed of wave-shaped rail wear in the direction of train motion (as a function of the number of axles of electric locomotives passed in traction mode) is directly proportional to the vertical load at the wheel and rail contact in the slip zone 0≤ Q ≤ F /(2 n ψ k ), is inversely proportional to wear resistance C and significantly depends on the parameters of the undercarriage of the electric train and the track superstructure.