研究目的
Investigating the influence of slit alignment and slit width on the luminosity measurement of arc discharge channel to establish the correlation between the current and the corresponding luminosity.
研究成果
The study demonstrates that proper alignment of the slit to the center of the discharge gap is crucial for accurate luminosity measurement. Improper alignment can lead to significant scatter and distortion in luminosity waveforms. The peak luminosity increases linearly with slit width, allowing for adjustment of luminosity signal output based on practical needs. These findings provide a foundation for future research on the correlation between current and luminosity in lightning channels.
研究不足
The study is limited to laboratory conditions with a 15-mm open-air gap between electrodes. The findings may not directly apply to natural lightning conditions. The slit width adjustment is effective only when the field of view does not exceed the entire length of the discharge channel.
1:Experimental Design and Method Selection:
A lightning channel luminosity detection system (LCLDS) was assembled to measure the luminosity of discharge channels created by impulse currents. The system includes an avalanche photodiode module, a neutral density filter, an extension tube, and an adjustable horizontal slit.
2:Sample Selection and Data Sources:
Impulse currents with different amplitudes and waveforms were produced in a 15-mm open-air gap between two graphite-rod electrodes.
3:List of Experimental Equipment and Materials:
The setup included an impulse current generator, a Pearson current monitor, a HBM ISOBE5500 isolation system, a Tektronix MDO 3024 oscilloscope, and a Nikon D3300 still camera.
4:Experimental Procedures and Operational Workflow:
The luminosity and current of the discharge channel were measured synchronously. The alignment of the slit and the slit width were varied to study their effects on luminosity measurement.
5:Data Analysis Methods:
The output signals of current and luminosity were recorded and analyzed for peak values, front times, and time to half-values.
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