I. Introduction
Measurements of partial discharge (PD) activity are a commonly used as a diagnostic tool to provide insight into the health of electrical insulation [1] . PD activity due to impulse voltage waveforms has recently received increased research attention [2 , 3] . The motivation for research this was the premature failure of electrical equipment that utilized these waveforms such as inverter fed motors [4] . PD measurements under impulse voltage waveforms in crossed-wire experiments have been shown to have higher apparent charge than sinusoidal waveforms [3] . PDs with a higher apparent charges are likely to cause more damage to insulation material and provide an explanation for the premature failure of the electrical equipment that uses impulse voltage waveforms. The reason for higher discharge magnitudes under impulse is thought to be that discharges regularly occur at voltages significantly above the inception voltage due to the quick rise times. It is also possible that in the crossed wire experiments high magnitude discharges can initiate other discharges leading to multiple PD events. The aim of this work is to provide insight into the discharge mechanisms of PD in crossed-wire experiments with the intention of providing qualitative insight into experimental measurements.