研究目的
To obtain the two dimensional density distribution of copper vapor in a forced vacuum arc extinction for understanding dielectric recovery processes, especially in DC interruptions.
研究成果
The LIF technique successfully provided two-dimensional distribution of copper vapor in forced vacuum arc extinction. For CuCr25 contacts, vapor was evenly distributed and decayed exponentially, dropping below 10% of initial density by 325 μs. For CuCr50 contacts, higher initial vapor density was observed with slower decay, suggesting that higher chromium content increases metal vapor production around current zero. This provides insights into dielectric recovery processes and supports further theoretical studies on DC interruptions.
研究不足
The fluorescence can only be detected after arc extinction due to strong arc radiation interference. The measurements are relative and not absolute densities. The study is limited to specific contact materials (CuCr25 and CuCr50) and may not generalize to other conditions. The fast-changing nature of DC interruptions makes precise observation challenging.
1:Experimental Design and Method Selection:
The study uses laser-induced fluorescence (LIF) technique to measure the density distribution of ground-state copper atoms in a vacuum arc extinction scenario. The principle involves exciting copper atoms with a laser at 324.8 nm and capturing fluorescence at 510.6 nm using an ICCD camera. The experimental circuit includes a main loop and a commutation loop to force the arc to current zero.
2:8 nm and capturing fluorescence at 6 nm using an ICCD camera. The experimental circuit includes a main loop and a commutation loop to force the arc to current zero. Sample Selection and Data Sources:
2. Sample Selection and Data Sources: The experiments are conducted using cylindrical contacts made of CuCr25 and CuCr50 materials with a diameter of 40 mm and a gap length of 15 mm in a demountable vacuum chamber pumped below 5 × 10^{-4} Pa.
3:List of Experimental Equipment and Materials:
Key equipment includes a dye laser (Quantel, wavelength
4:8 nm, pulse width 5 ns, frequency 10 Hz, energy 5 mJ), an ICCD camera (Andor iStarDH334T, 1024 × 1024 pixels), a band-pass filter (center wavelength 32 nm, bandwidth 84 nm), capacitors (C
3 100 mF, C2: 2 mF), inductor (L1: 0.1 mH), thyristor, high-voltage probe, Hall-current sensor, oscilloscope, and vacuum chamber with quartz windows.
5:1 mH), thyristor, high-voltage probe, Hall-current sensor, oscilloscope, and vacuum chamber with quartz windows. Experimental Procedures and Operational Workflow:
4. Experimental Procedures and Operational Workflow: The main capacitor is charged to 50 V and the reverse capacitor to 100 V. A vacuum arc is initiated by a trigger electrode, and after 5 ms, the thyristor is triggered to force current zero. The laser is fired at specific time intervals (from 125 μs to 375 μs with 25 μs steps) after arc extinction, and the ICCD captures fluorescence signals with a 50 ns exposure time.
6:Data Analysis Methods:
The fluorescence intensity is analyzed to determine the relative density distribution of copper vapor, assuming proportionality between fluorescence photons and ground-state atom density. Temporal evolution is plotted to observe decay patterns.
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dye laser
Quantel
Quantel
To emit a laser beam for exciting copper atoms in the LIF technique.
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ICCD
iStarDH334T
Andor
To capture the fluorescence signal from the vacuum arc plasma.
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band-pass filter
To eliminate arc light by filtering for the fluorescence wavelength.
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capacitor
C1
Part of the main loop to generate arc current.
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capacitor
C2
Part of the commutation loop to inject counter-current.
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inductor
L1
Part of the main loop to shape the current waveform.
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thyristor
To switch the commutation loop for forcing current zero.
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high-voltage probe
To measure the vacuum arc voltage.
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Hall-current sensor
To measure the arc current.
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oscilloscope
To record voltage and current data.
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