正交磁场对电火花单脉冲放电中电蚀凹坑的影响规律

Effects of an orthogonal magnetic field on discharge craters created during the single-spark electrical discharge machining process

  • 摘要: 电火花放电通道在正交磁场的作用下向洛伦兹力方向偏转、延伸,进而导致电蚀凹坑形貌发生变化,研究磁场辅助电火花加工(MF-EDM)过程中电蚀凹坑的形貌变化规律及特点,对进一步明晰电火花加工机理具有重要意义. 基于MF-EDM气中单脉冲放电试验,使用表面轮廓仪观测电蚀凹坑延伸长度、深度、宽度及放电起始点偏移量,并得出磁场及放电参数对电蚀凹坑的影响规律. 结果表明:电蚀凹坑长度随着磁感应强度、开路电压的增大而增大;电极外伸长度的影响结果相反;电蚀凹坑深度随着磁感应强度、开路电压、电极外伸长度的增加没有明显的变化规律;电容与磁感应强度存在最优参数组合以使凹坑长度最大;随着磁感应强度及放电能量的增加放电起始点的偏移量增加.

     

    Abstract: In the single-spark electrical discharge machining (EDM) process under the action of an orthogonal magnetic field, the plasma from the electric discharge is deflected and extends to the direction of the Lorenz force, which leads to a change in the discharge craters compared with traditional EDM. In this paper, the morphology and characteristics of craters created during the process of magnetic field assisted electrical discharge machining (MF-EDM) were studied. The results of this study may be applied to production practice, and it is expected that the machining of tapered holes can be realized using magnetic field assisted EDM. Based on single-pulse MF-EDM in gas, the crater morphology was observed using a surface topography instrument. During the experiment the voltage waveform was obtained using an oscilloscope and the current waveform was calculated using the simulation software SABER. After measuring the distribution of the orthogonal magnetic field, the ampere force of the electrode at the moment of discharge was calculated. The deformation of the end of the electrode was obtained using simulation software ANSYS15.0. The offset of the starting point of the discharge under the influence of the orthogonal magnetic field was proven. Then, rules for the effects of the magnetic field and discharge parameters on the craters were obtained. The results indicate that crater length increases with an increase in magnetic field intensity and open circuit voltage, but the influence of the electrode overhang length shows the opposite. There is no obvious change rule for crater depth with an increase in magnetic field intensity, open circuit voltage, or electrode overhang length. To obtain the maximum length or minimum depth of the crater, an optimum combination of the capacitance and magnetic field intensity can be used. With an increase in magnetic induction intensity and discharge energy, the offset of the discharge point increases.

     

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