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Characterization of Contact Discharge Between Small-Capacitance Devices

机译:小型电容设备之间的接触放电特性

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The giant-magnetoresistive head suffers magnetic damage from electrostatic discharge (ESD) current on the order of 10 mA and thermal damage from ESD energy on the order of 0.5 nJ. The discharge between 2-pF capacitors at 10 V gave a peak current of 34 mA, and the discharge between 100-pF capacitors at 100 V reached 1.5 A. The peak current arose on the order of picofarads and was approximately maximized at the same value of both capacitors. Theoretical energy loss was estimated by the difference between the potential energies prior to and following the discharges. The energy loss was 0.05 nJ for 2-pF capacitors at 10 V and increased in excess of 0.5 nJ for greater than 20-pF capacitors. Therefore, the discharge between picofarad capacitances tends to cause the magnetic damage, and increasing the capacitance causes the thermal damage. Comparison of the potential energy loss and the current energy derived that the contact resistance varied from more than 200 $Omega$ to few ohms as the voltage and the energy loss increased.
机译:巨磁阻磁头因静电放电(ESD)电流而遭受的磁损坏约为10 mA,而由于ESD能量而遭受的热损坏约为0.5 nJ。在10 V电压下2 pF电容器之间的放电产生了34 mA的峰值电流,而在100 V电压下100 pF电容器之间的放电达到了1.5A。该峰值电流出现在皮法级的数量级,并且在相同值下近似最大化。两个电容器。理论能量损失是通过放电前后的势能之差估算的。对于10 pV的2 pF电容器,能量损耗为0.05 nJ,而对于大于20 pF的电容器,能量损耗增加超过0.5 nJ。因此,皮法拉电容之间的放电趋于引起磁损坏,而增大电容会引起热损坏。比较潜在的能量损失和电流能量可以得出,随着电压和能量损失的增加,接触电阻从200Ω以上变化到几欧姆。

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