1996
DOI: 10.1088/0963-9659/5/4/011
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Spectroscopic measurements of radial distribution of electron density and temperature in a plasma

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“…One type of the images showed that the electron densities in the cathode tip vicinity (CTV) were locally reduced below our sensors sensitivity of 10 21 m −3 and the electron density distributions in the axial direction y were seen to be spatially discontinuous, as shown in figure 11(a). The electron densities in −0.9 y 1.5 mm were 10 22−23 m −3 , which agreed well with the electron densities at the current-zero point for a puffer-type SF 6 gas circuit breaker observed by using Stark broadening [39]. Figure 11(b) shows that the simultaneously recorded voltage and current waveforms had damping rates of dv/dt = 0.42 kV μs −1 and di/dt = 0.27 A μs −1 around the current-zero point, respectively.…”
Section: Sf 6 Gas-blastsupporting
confidence: 82%
“…One type of the images showed that the electron densities in the cathode tip vicinity (CTV) were locally reduced below our sensors sensitivity of 10 21 m −3 and the electron density distributions in the axial direction y were seen to be spatially discontinuous, as shown in figure 11(a). The electron densities in −0.9 y 1.5 mm were 10 22−23 m −3 , which agreed well with the electron densities at the current-zero point for a puffer-type SF 6 gas circuit breaker observed by using Stark broadening [39]. Figure 11(b) shows that the simultaneously recorded voltage and current waveforms had damping rates of dv/dt = 0.42 kV μs −1 and di/dt = 0.27 A μs −1 around the current-zero point, respectively.…”
Section: Sf 6 Gas-blastsupporting
confidence: 82%