轮轨波磨形成机理与再现试验
M echanism and ExperimentalFormation ofW heel/RailCorrugation
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摘要: 根据非线性振动理论和赫兹理论,分析了钢轨波磨与轮轨纵向自激振动幅值和接触椭圆纵向轴长的关 系.分析表明,钢轨波磨产生的机理是轮对自激振动幅值大于接触椭圆纵向轴长;对于实际的轮轨系统,波磨产 生的条件是轮对横移量大于临界值.据此,对波磨形成的过程进行了仿真计算并设计了再现试验。计算结果表 明,在轮对横移量为8 mm时,接触表面产生短波长(16~20 mm)波磨.再现试验用机车轮对在滚动振动试验台 上进行.当横移量为8和11 mm时,均产生波磨.前者波长均匀,约20 mm;后者波长不均匀,在18~27 mm之间. 横移量为6 mm时无明显波磨.仿真计算和试验均支持关于波磨产生的机理和条件的结论.Abstract: The relationship betweenwheel/rail(W /R) corrugation and thewavelength of longitudinal self-vibration and the longitudinal axis of contactellipsewas analyzed based on the nonlinear vibration and Hertzian theories. The analysis shows that the mechanism of W /R corrugation is that the wavelength of longitudinal self-vibration is larger than the longitudinal axis ofcontactellipse; for a real W /R system, the criterion is that the lateral displacement of the wheelset is larger than a critical value. Numerical simulation and testwere conducted to verify the proposedmechanism and criterion. The simulation results show thatcorrugationswith lengthsbetween 16 to20mm appearwhen the lateral displacementof thewheelset is 8 mm. Corrugation testwas conducted on a rolling vibration test rig. Corrugations form when the lateraldisplacements of thewheelsetare 8 and 11mm, and the lengths are about20 mm and 18 to 27 mm, respectively, under the former and the latter conditions. There is no obvious corrugationwhen the lateral displacement is 6 mm.
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Key words:
- wheel/rail contact /
- corrugation /
- cyclicwear /
- contactvibration
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