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...

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Main Authors: Teck Seng Ho, Christine Charles, Roderick W. Boswell
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
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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
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