Effect of Discharge Plasma Potential on Diffusion Plasma Parameters Controlled by a Mesh Grid in a Double Plasma Device

2013 ◽  
Vol 53 (3) ◽  
pp. 206-213 ◽  
Author(s):  
M. K. Mishra ◽  
A. Phukan ◽  
M. Chakraborty
Keyword(s):  
Discharge Plasma ◽  
Plasma Potential ◽  
Plasma Parameters ◽  
Plasma Device ◽  
Double Plasma Device ◽  
Mesh Grid

Effect of discharge voltage on bi-Maxwellian electrons in the diffusion plasma region of a double plasma device

2013 ◽  
Vol 79 (5) ◽  
pp. 913-920
Author(s):  
M. K. MISHRA ◽  
A. PHUKAN ◽  
M. CHAKRABORTY
Keyword(s):  
Probability Function ◽  
Energetic Electron ◽  
Plasma Potential ◽  
Discharge Voltage ◽  
Diffusion Region ◽  
Plasma Region ◽  
Temperature Plasma ◽  
Plasma Device ◽  
Double Plasma Device ◽  
Mesh Grid

AbstractThe effect of discharge voltage on bi-Maxwellian electrons in the diffusion region of a double plasma device has been studied. The increase in discharge voltage enhances the flux of ionizing electrons to the diffusion region separated by a mesh grid. This energetic electron flux in turn affects other important parameters such as density, electron temperature, plasma potential and floating potential in the diffusion region. Furthermore, the dependence of density and temperature of both ionizing and plasma electrons on discharge voltage is investigated. The electron energy probability function obtained from probe data also indicates the bi-Maxwellian nature of electrons.

WITHDRAWN: Role of high energetic electrons in controlling diffused plasma parameters in a double plasma device

2007 ◽  
Author(s):  
M.K. Mishra ◽  
A. Phukan ◽  
M. Chakraborty ◽  
K.S. Goswami
Keyword(s):  
Plasma Parameters ◽  
Energetic Electrons ◽  
Plasma Device ◽  
Double Plasma Device

Plasma parameters controlled by remote electron shower in a double plasma device

2012 ◽  
Vol 38 (7) ◽  
pp. 590-594 ◽  
Author(s):  
M. K. Mishra ◽  
A. Phukan
Keyword(s):  
Plasma Parameters ◽  
Plasma Device ◽  
Double Plasma Device ◽  
Electron Shower

Role of high energetic electrons in controlling diffused plasma parameters in a double plasma device

2007 ◽  
Vol 365 (1-2) ◽  
pp. 135-139 ◽  
Author(s):  
M.K. Mishra ◽  
A. Phukan ◽  
M. Chakraborty ◽  
K.S. Goswami
Keyword(s):  
Plasma Parameters ◽  
Energetic Electrons ◽  
Plasma Device ◽  
Double Plasma Device

Mechanical variations of diffused plasma parameters in a double plasma device

2007 ◽  
Vol 40 (12) ◽  
pp. 3616-3619 ◽  
Author(s):  
Arindam Phukan ◽  
Mrinal Kr Mishra ◽  
Monojit Chakraborty
Keyword(s):  
Plasma Parameters ◽  
Plasma Device ◽  
Double Plasma Device

Variations of Plasma Parameters and Sheath Thickness Due to the Extraction of Ion and Electron Flux in a Double Plasma Device

2007 ◽  
Vol 47 (10) ◽  
pp. 703-709 ◽  
Author(s):  
M. K. Mishra ◽  
A. Phukan ◽  
M. Chakraborty
Keyword(s):  
Electron Flux ◽  
Sheath Thickness ◽  
Plasma Parameters ◽  
Plasma Device ◽  
Double Plasma Device

Variation of plasma parameters in a modified mode of plasma production in a double plasma device

Pramana ◽  
2010 ◽  
Vol 74 (3) ◽  
pp. 399-409 ◽  
Author(s):  
A. Phukan ◽  
M. K. Mishra ◽  
B. K. Saikia ◽  
M. Chakraborty
Keyword(s):  
Plasma Parameters ◽  
Plasma Production ◽  
Plasma Device ◽  
Double Plasma Device

Reflection of ion-acoustic waves from bipolar potential structures

1989 ◽  
Vol 41 (2) ◽  
pp. 243-255 ◽  
Author(s):  
Y. Nakamura ◽  
Joyanti Chutia
Keyword(s):  
Acoustic Wave ◽  
Acoustic Waves ◽  
High Efficiency ◽  
Ion Beam ◽  
Plasma Potential ◽  
Ion Acoustic Waves ◽  
Ion Acoustic Wave ◽  
Plasma Device ◽  
Ion Acoustic ◽  
Double Plasma Device

Reflection of ion-acoustic waves from the ion sheath in front of the separation grid in a double-plasma device has been investigated experimentally. The plasma potential φ of the source plasma was controlled relative to that of the target plasma. When eφ < κΤe, where Τe is the electron temperature, no reflection was observed. The reason for this is that ions are drifting towards the grid with the Bohm velocity, i.e. the ion-acoustic velocity. When eφ > κΤe the reflected wave consists of the ion-acoustic wave and the ion beam mode. The reflection coefficient for the ion-acoustic wave is about unity. This high efficiency is due to reflection of the ions themselves.

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