Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation
A computational fluid dynamics and plasma model of a collisional (~ a few Torr) radiofrequency (at 13.56 MHz) argon plasma capacitively coupled in a converging-diverging nozzle (applied to the optimization of electrothermal plasma thrusters for space use) shows the formation of a strong stationary c...
Main Authors: | , , |
---|---|
Format: | Article |
Language: | English |
Published: |
Frontiers Media S.A.
2019-11-01
|
Series: | Frontiers in Physics |
Subjects: | |
Online Access: | https://www.frontiersin.org/article/10.3389/fphy.2019.00200/full |
id |
doaj-7a3c127132b14ab38f87a1cd2eeef4cb |
---|---|
record_format |
Article |
spelling |
doaj-7a3c127132b14ab38f87a1cd2eeef4cb2020-11-25T02:17:53ZengFrontiers Media S.A.Frontiers in Physics2296-424X2019-11-01710.3389/fphy.2019.00200493593Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle SimulationTeck Seng HoChristine CharlesRoderick W. BoswellA computational fluid dynamics and plasma model of a collisional (~ a few Torr) radiofrequency (at 13.56 MHz) argon plasma capacitively coupled in a converging-diverging nozzle (applied to the optimization of electrothermal plasma thrusters for space use) shows the formation of a strong stationary current-free double layer (CFDL) at the 1.5 mm diameter nozzle throat for a downstream pressure of ~ 0.1 Torr. The cycle average magnitude of the double layer potential is ΔΦDL = 77 V and the electron temperature at the high potential edge of the double layer is kBTe = 2.64 eV, yielding a strength of ΔΦDL/(kBTe) ~ 30. The double layer is 1.2 mm wide which corresponds to ~ 90 Debye lengths. The axial electric field of the double layer accelerates ions along the nozzle to a maximum drift velocity of 17 km s−1, about 3.3 times the ion sound speed, and their kinetic energy is transferred to neutrals by ion-neutral charge exchange collisions. The ion transit time τi through the potential structure spontaneously forming at the nozzle throat is about 5 times the radiofrequency excitation period τRF. These findings are discussed in the broader context of double layer physics and the dynamics of their formation as well as in the context of electrothermal thruster optimization in which neutral propellant heating via ion-neutral charge exchange collisions is the main source of thrust.https://www.frontiersin.org/article/10.3389/fphy.2019.00200/fullplasma simulationplasma nozzlethrusterdouble layerion acceleration |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Teck Seng Ho Christine Charles Roderick W. Boswell |
spellingShingle |
Teck Seng Ho Christine Charles Roderick W. Boswell Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation Frontiers in Physics plasma simulation plasma nozzle thruster double layer ion acceleration |
author_facet |
Teck Seng Ho Christine Charles Roderick W. Boswell |
author_sort |
Teck Seng Ho |
title |
Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation |
title_short |
Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation |
title_full |
Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation |
title_fullStr |
Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation |
title_full_unstemmed |
Current-Free Electric Double Layer in a Small Collisional Plasma Thruster Nozzle Simulation |
title_sort |
current-free electric double layer in a small collisional plasma thruster nozzle simulation |
publisher |
Frontiers Media S.A. |
series |
Frontiers in Physics |
issn |
2296-424X |
publishDate |
2019-11-01 |
description |
A computational fluid dynamics and plasma model of a collisional (~ a few Torr) radiofrequency (at 13.56 MHz) argon plasma capacitively coupled in a converging-diverging nozzle (applied to the optimization of electrothermal plasma thrusters for space use) shows the formation of a strong stationary current-free double layer (CFDL) at the 1.5 mm diameter nozzle throat for a downstream pressure of ~ 0.1 Torr. The cycle average magnitude of the double layer potential is ΔΦDL = 77 V and the electron temperature at the high potential edge of the double layer is kBTe = 2.64 eV, yielding a strength of ΔΦDL/(kBTe) ~ 30. The double layer is 1.2 mm wide which corresponds to ~ 90 Debye lengths. The axial electric field of the double layer accelerates ions along the nozzle to a maximum drift velocity of 17 km s−1, about 3.3 times the ion sound speed, and their kinetic energy is transferred to neutrals by ion-neutral charge exchange collisions. The ion transit time τi through the potential structure spontaneously forming at the nozzle throat is about 5 times the radiofrequency excitation period τRF. These findings are discussed in the broader context of double layer physics and the dynamics of their formation as well as in the context of electrothermal thruster optimization in which neutral propellant heating via ion-neutral charge exchange collisions is the main source of thrust. |
topic |
plasma simulation plasma nozzle thruster double layer ion acceleration |
url |
https://www.frontiersin.org/article/10.3389/fphy.2019.00200/full |
work_keys_str_mv |
AT tecksengho currentfreeelectricdoublelayerinasmallcollisionalplasmathrusternozzlesimulation AT christinecharles currentfreeelectricdoublelayerinasmallcollisionalplasmathrusternozzlesimulation AT roderickwboswell currentfreeelectricdoublelayerinasmallcollisionalplasmathrusternozzlesimulation |
_version_ |
1724884509150674944 |