2014
DOI: 10.1002/eej.22635
|View full text |Cite
|
Sign up to set email alerts
|

Measurements of Electron Density and Electron Temperature of Arc Discharge Plasmas Containing Metallic Vapors Using Laser Thomson Scattering

Abstract: Laser Thomson scattering (LTS) was applied to arc discharges generated in the atmosphere to measure electron density (n e ) and electron temperature (T e ). The electrode gap was 0.8 mm, and the electrode diameter was 1 mm. The applied voltage was 6 kV, the peak current was 600 A, and the decay time of the voltage and current was 25 μs. The spatiotemporal evolution of n e and T e was measured 10, 30, and 50 μs after discharge initiation. At these times, the obtained values of n e and T e were estimated to be i… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2

Citation Types

0
2
0

Year Published

2022
2022
2024
2024

Publication Types

Select...
3
1

Relationship

0
4

Authors

Journals

citations
Cited by 4 publications
(2 citation statements)
references
References 22 publications
0
2
0
Order By: Relevance
“…The Thomson scattering (TS) spectrum is a measure of the electron velocity distribution function, and it provides direct measurement of electron density and temperature with minimal assumptions on plasma conditions, such as symmetry, composition, and equilibrium. LTS has been widely implemented in high-temperature nuclear fusion plasmas, but has recently expanded its applications in various low-temperature plasma sources, including glow discharge 24 , arc discharge 25 , microwave discharge 26 , 27 , nanosecond pulsed discharge 28 , plasma jets 29 , and laser-induced plasmas 30 33 . When employing TS for low-temperature plasmas, it is essential to consider the effect that the probing laser has on the plasma itself.…”
Section: Introductionmentioning
confidence: 99%
“…The Thomson scattering (TS) spectrum is a measure of the electron velocity distribution function, and it provides direct measurement of electron density and temperature with minimal assumptions on plasma conditions, such as symmetry, composition, and equilibrium. LTS has been widely implemented in high-temperature nuclear fusion plasmas, but has recently expanded its applications in various low-temperature plasma sources, including glow discharge 24 , arc discharge 25 , microwave discharge 26 , 27 , nanosecond pulsed discharge 28 , plasma jets 29 , and laser-induced plasmas 30 33 . When employing TS for low-temperature plasmas, it is essential to consider the effect that the probing laser has on the plasma itself.…”
Section: Introductionmentioning
confidence: 99%
“…Thus, to detect Raman and Thomson scattering signals, the light near the laser line (Rayleigh scattering/stray light) should be effectively removed to prevent saturation of the detector. Such laser line rejection can be performed with multiple techniques such as a triple grating spectrograph [4][5][6][7][8][9][10][11][12], a vapor cell [13][14][15], a glass/interference filter [16], a physical mask [17,18], and a volume Bragg grating (VBG) filter [19][20][21][22][23][24][25][26].…”
Section: Introductionmentioning
confidence: 99%