由于粗糙表面的微动腐蚀,电连接器中的电阻增加

M. D. Bryant
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引用次数: 69

摘要

建立了一个全面的模型来预测第n次微动周期的接触电阻和接触的最终使用寿命。该模型包含接触擦拭,微动振动幅度和频率,污染物化学,材料特性,镀层厚度,粗糙变形,正常负载,电负载和表面形貌。假设微动振动使接触的杂质分离,使原始的金属a点暴露于环境污染物的攻击之下。该模型计算了在微动循环的分离阶段在暴露表面上产生的腐蚀产物的量。当微动运动将暴露在外的腐蚀凸起拉回一起时,尺寸不匹配就会发生,一些腐蚀性产物被刮掉并沉积在山谷中。最终,山谷填充并分离了a点,导致“最终”失败。产生量和刮去量之间的物质平衡估计了被拖入接触的腐蚀性产物的量。分子通过塑性变形的转移,将腐蚀性产物的颗粒混合到粗糙的金属中。将混合与塑性流动相关联的假设和现代复合材料理论的使用导致了对污染粗糙体内电导率的估计。对粗糙体进行积分得到粗糙体阻力,并应用Greenwood理论估计总接触阻力。结果表明,接触电阻随时间单调增加。最初增长缓慢,随后迅速增长。预测的故障时间与现场测量结果一致。
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Resistance buildup in electrical connectors due to fretting corrosion of rough surfaces
A comprehensive model to predict the contact resistance during the nth fretting cycle and the ultimate usable lifetime of the contact has been developed. This model incorporates contact wipe, fretting vibration amplitude and frequency, contaminant chemistry, material properties, plating thickness, asperity deformations, normal load, electrical load, and surface topography. It is assumed that fretting vibrations separate contacting asperities and expose virgin metallic a-spots to environmental contaminant attack. The model calculates the amount of corrosive product produced on the exposed surfaces during the separation phase of a cycle of fretting. As fretting motions pull the exposed corroded asperities back together, a mismatch in size occurs and some of the corrosive product is scraped off and deposited in the valleys. Eventually, the valleys fill and separate the a-spots, resulting in "ultimate" failure. A material balance between amounts produced and scraped off estimates the amount of corrosive product dragged into the contact. Shifting of molecules via plastic deformation mix particles of corrosive product into the asperity metal. Assumptions that correlate mixing to plastic flow and use of modern composite theory leads to an estimate of the conductivity within the contaminated asperity. Integration over the asperity volume gives the asperity resistance, and application of Greenwood's theory estimates the total contact resistance. Results show a monotonic increase in contact resistance over time. Initial increases are slow, followed by rapid increases. Predicted failure times are consistent with field measurements.
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