用有限元模型指示盘式制动器更换临界厚度时摩擦温度与磨损的一致性

Eric Amoah Asante, Michael Adusei-Bonsu, Randy Amuaku, E. Ampaw
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引用次数: 0

摘要

厚度的减少降低了制动盘的散热能力和机械强度,引发了一系列的关键故障和失效。为了确定换盘的临界厚度,采用有限元方法对有摩擦热的盘式制动器接触问题进行了瞬态分析。为了分析制动盘厚度对摩擦热产生的影响,设计了制动盘厚度为5.0 mm、5.5 mm、6.0 mm、6.5 mm、7.0 mm、7.5 mm和8.0 mm的不同制动盘模型。随后,在2210 N、2875 N和3538 N制动力以及884 rpm、1149 rpm和1415 rpm转速下,对所开发的制动盘模型进行了评估。利用SolidWorks有限元分析软件对盘式制动器在重复制动工况下的热弹性行为进行了数值模拟。结果表明,当制动力由2210 N增加到2875 N、2875 N增加到3538 N、2210 N增加到3538 N时,变形量分别为28.45%、33.62%和52.5%。随后,将圆盘转速从884 rpm增加到1149 rpm、1149 rpm增加到1415 rpm、884 rpm增加到1415 rpm,变形率分别为69.57%、17.23%和74.8%。虽然,在连续力的差异是相同的,百分比的变形是不一样的,而是下降的增加。在极限应力情况下,在相同制动力为2210牛的情况下,施加884转/分、1149转/分和1415转/分的转速分别产生了1.327 × 1011 N/m2、2.069 × 1011 N/m2和2.072 × 1011 N/m2的极限应力。将制动盘转速从884转/分提高到1149转/分和从1149转/分提高到1415转/分时,极限应力分别为35.86%和0.14%。总体结果表明,在相同的处理条件下;制动力效应>盘转速效应>盘厚效应。在读取读数的所有半径点上,温度都急剧下降,这可能是由于在接触时从磁盘到垫的初始热量传递。最小厚度为最佳的热量和磨损减少6.7毫米。本文的研究为盘式制动系统的设计提供了有益的工具,提高了盘式制动系统的制动性能。
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Consistency of Frictional Temperature and Wear on Indicating the Critical Thickness for Disc Brake Replacement by Finite Element Model
Reduced thickness reduces the heat dissipation capacity of the brake disc and its mechanical strength, triggering a series of critical faults and failures. To determine the critical thickness for disc replacement, a transient analysis for contact problem of disc brakes with frictional heat was performed using finite element method. To analyze the effect of disc thickness on the frictional heat generation, different brake disc models were developed with disc thicknesses of 5.0 mm, 5.5 mm, 6.0 mm, 6.5 mm, 7.0 mm, 7.5 mm and 8.0 mm. Subsequently, the developed disc models were evaluated under 2210 N, 2875 N and 3538 N braking forces and 884 rpm, 1149 rpm and 1415 rpm rotational speed of the disc. The numerical simulation for the thermoelastic behavior of disk brake was obtained in the repeated brake condition by Finite Element Analysis package of SolidWorks. The results showed that increasing the braking force from 2210 N to 2875 N, 2875 N to 3538 N and 2210 N to 3538 N resulted in 28.45%, 33.62% and 52.5% deformations respectively. Subsequently, increasing the rotational speed of the disc from 884 rpm to 1149 rpm, 1149 rpm to 1415 rpm and 884 rpm to 1415 rpm resulted in 69.57%, 17.23% and 74.8% deformations respectively. Though, the differences in successive forces is the same, the percentage deformation was not the same but rather a decline in the increase. In the case of the ultimate stress, the application of 884 rpm, 1149 rpm and 1415 rpm speeds at the same braking force of 2210 N yielded 1.327 x 1011 N/m2, 2.069 x 1011 N/m2 and 2.072 x 1011 N/m2 ultimate stresses respectively. Increasing the rotational speed of the brake disc from 884 rpm to 1149 rpm and 1149 rpm to 1415 rpm resulted in 35.86% and 0.14% ultimate stress respectively. The overall results have shown that, under the same condition of treatment; effect of braking force > effect disc rotational speed > effect of disc thickness. There was a sharp drop in temperature at all the radii points where readings were taken and this could be due to initial heat transfer from the disc to the pad just at contact. The minimum thickness for optimal heat and wear reduction 6.7 mm. The present study can provide a useful design tool and improve the brake performance of disk brake system.
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