Examines wheel climb assumptions, revealing complex dynamics affecting derailment criteria.
In railroad wheel climb L / L V . -0pt V L L V V derailment criteria, it is assumed that the direction of the relative velocity of the flange-contact point in its totality is downward, leading to an upward friction force along the wheel flange profile. That is, the longitudinal component of the relative velocity of the flange-contact point is assumed negligible. It is further assumed that the climb progresses along a flange profile, and consequently, the flange-contact point trajectory is defined by the flange profile curve or a straight line. This paper examines these two basic assumptions by developing a three-dimensional wheel climb model that relaxes the assumptions used in deriving the planar L / L V . -0pt V L L V V ratio. The results obtained show that, in case of flange contact at a large angle of attack, there is a nonzero longitudinal velocity component of the wheel flange-contact point, and the trajectory of this point is not, in general, defined by the flange profile or a straight line. Consequently, the phenomenon of wheel climb at a large angle of attack is three-dimensional, demonstrating the need for further investigations of the derailment criteria based on planar analysis.
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Shabana et al. (2026) studied this question.
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