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Experiments and Modeling of Gas Heating in a Radio-Frequency Plasma Jet

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Small plasma sources have been developed for a variety of applications and are often known as plasma jets (e.g. biomedical applications using atmospheric pressure helium or argon plasmas), as micro-plasma sources or arrays [1] (e.g. surface processing using lower operating pressure plasmas), or as micro-thrusters (e.g. electric propulsion using hollow cathode thrusters or neutralizers). At the ANU we have designed a capacitively coupled radiofrequency (13.56 MHz) cylindrical plasma source which currently operates at pressures around a few Torr and at powers ranging from 1-100 Watts with or without a pressure gradient imposed along the 2 cm long cavity [2]. The plasma diameter ranges from 1 to 6 mm before expanding in a larger chamber. Neutral gas heating is measured for a variety of gases (argon, nitrogen, xenon) and cavity diameters using optical emission spectroscopy. The results are combined with electric probe measurements to develop a plasma heating model where the heating is assumed to come from ion-neutral collisions in the maximum of the discharge under the powered electrode. A peaked density on axis is well described by the plasma model [2]. Typically, gas temperatures around 1000K are measured for N2 and Ar in agreement with theoretical predictions from Fruchtman [3]. The results show that this type of source can be tailored to suit a variety of plasma applications: its effectiveness in dissociating species means that it can be used for remote plasma etching [1] or for surface passivation from atomic nitrogen using N2. It can also be developed as an electrothermal plasma micro-thruster for space propulsion[2]. All of these applications benefit from the neutral gas heating and from the ability of the source to be developed as an array of sources. REFERENCES: [1]S. Dixon, C. Charles, R. Boswell, W. Cox, J. Holland and R. Gottscho, “Interactions between arrayed hollow cathodes”, J. Phys. D: Appl. Phys. 46, 145204, 2013 [2]C. Charles and R.W. Boswell, “Measurement and modeling of a radiofrequency micro-thruster”, Plasma Sources Sci. Technol. 21, 022002, 2012 [3]A. Fruchtman, “Energizing and depletion of neutrals by a collisional plasma”, Plasma Sources Sci. Technol. 21, 022002, 2012
Title: Experiments and Modeling of Gas Heating in a Radio-Frequency Plasma Jet
Description:
Small plasma sources have been developed for a variety of applications and are often known as plasma jets (e.
g.
biomedical applications using atmospheric pressure helium or argon plasmas), as micro-plasma sources or arrays [1] (e.
g.
surface processing using lower operating pressure plasmas), or as micro-thrusters (e.
g.
electric propulsion using hollow cathode thrusters or neutralizers).
At the ANU we have designed a capacitively coupled radiofrequency (13.
56 MHz) cylindrical plasma source which currently operates at pressures around a few Torr and at powers ranging from 1-100 Watts with or without a pressure gradient imposed along the 2 cm long cavity [2].
The plasma diameter ranges from 1 to 6 mm before expanding in a larger chamber.
Neutral gas heating is measured for a variety of gases (argon, nitrogen, xenon) and cavity diameters using optical emission spectroscopy.
The results are combined with electric probe measurements to develop a plasma heating model where the heating is assumed to come from ion-neutral collisions in the maximum of the discharge under the powered electrode.
A peaked density on axis is well described by the plasma model [2].
Typically, gas temperatures around 1000K are measured for N2 and Ar in agreement with theoretical predictions from Fruchtman [3].
The results show that this type of source can be tailored to suit a variety of plasma applications: its effectiveness in dissociating species means that it can be used for remote plasma etching [1] or for surface passivation from atomic nitrogen using N2.
It can also be developed as an electrothermal plasma micro-thruster for space propulsion[2].
All of these applications benefit from the neutral gas heating and from the ability of the source to be developed as an array of sources.
REFERENCES: [1]S.
Dixon, C.
Charles, R.
Boswell, W.
Cox, J.
Holland and R.
Gottscho, “Interactions between arrayed hollow cathodes”, J.
Phys.
D: Appl.
Phys.
46, 145204, 2013 [2]C.
Charles and R.
W.
Boswell, “Measurement and modeling of a radiofrequency micro-thruster”, Plasma Sources Sci.
Technol.
21, 022002, 2012 [3]A.
Fruchtman, “Energizing and depletion of neutrals by a collisional plasma”, Plasma Sources Sci.
Technol.
21, 022002, 2012.

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