atmospheric pressure plasma transfer of jets and bullets across dielectric tubes and channels*
DESCRIPTION
ATMOSPHERIC PRESSURE PLASMA TRANSFER OF JETS AND BULLETS ACROSS DIELECTRIC TUBES AND CHANNELS* Zhongmin Xiong (a) , Eric Robert (b) , Vanessa Sarron (b) Jean-Michel Pouvesle (b) , Mark J. Kushner (a) (a) University of Michigan Department of Electrical Engineering and Computer Sciences - PowerPoint PPT PresentationTRANSCRIPT
ATMOSPHERIC PRESSURE PLASMA TRANSFER OF JETS AND BULLETS ACROSS DIELECTRIC TUBES
AND CHANNELS*
Zhongmin Xiong(a), Eric Robert(b), Vanessa Sarron(b)
Jean-Michel Pouvesle(b), Mark J. Kushner(a)
(a) University of MichiganDepartment of Electrical Engineering and Computer Sciences
Ann Arbor, MI [email protected], [email protected]
(b) GREMI, CNRS-Polytech’Orléans, 45067 Orléans Cedex 2, France
[email protected], [email protected] [email protected]
65th Gaseous Electronics Conference 2012, Austin, Texas, USA
* Work at UoM is supported by the DOE OFES and NSF. Work at GREMI is supported through APR "Plasmed" and ANR Blanc "PAMPA"
Experimental studies of atmospheric pressure plasma transfer across two perpendicular dielectric tubes.
Numerical modeling of atmospheric pressure plasma transfer across
two perpendicular dielectric channels
Primary ionization wave (IW) with positive polarity: Top-down transfer process, polarity preserving
Primary IW with negative polarity: Bottom-up transfer process, polarity reversing
Effects of rise-time of the primary IW
Concluding Remarks
AGENDA
University of MichiganInstitute for Plasma Science & Engr.GEC2012
PLASMA TRANSFER EXPERIMENTS
University of MichiganInstitute for Plasma Science & Engr.
E. Robert et al (GREMI, 2011)
X. Lu et al, J. Appl. Phys. 105, 043304 (2009)
GEC2012V. Johnson et al, IEEE TPS 39, 2360 (2011)
Atmospheric pressure plasma transfer refers to the production of an ionization wave (IW) in a tube or channel by impingement on the outer surface of a separately produced IW.
S. Wu et al, IEEE TPS 39, 2292 (2011)
PLASMA TRANSFER POSITIVE POLARITY
University of MichiganInstitute for Plasma Science & Engr.
E. Robert et al (GREMI, 2011)
Neon plasma, atmospheric pressure, 10 ns snapshots, filament penetration
No« thin plasma layer »
« filaments » across the transfer pipe
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PLASMA TRANSFER NEGATIVE POLARITY
University of MichiganInstitute for Plasma Science & Engr.
E. Robert et al (GREMI, 2011)
« thin plasma layer »
« thin plasma layer »
plasma « plume »
Neon plasma, atmospheric pressure, 10 ns snapshots Formation of thin plasma layer in the transfer tube
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TWO DIMENSIONAL PLASMA MODELING
University of MichiganInstitute for Plasma Science & Engr.
Channels filled with Ne/Xe = 99.9/0.1
Channels 4 mm wide, separated by 4 mm in air.
25 kV pulse of either polarity is applied on the powered electrode.
The pulse rise-time varies from 25 to 400 ns. The pulse duration is 100 ns.
Initial electron density [e] in the lower (transfer) channel is [e]0 = 1 x 107 (cm-3).
Surrounding air is treated as dielectric material ( = 1).
The mole fraction of neon is computed using ANSYS FLUENT v.12.0.
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MODELING PLATFORM: nonPDPSIM Poisson’s equation:
Transport of charged and neutral species:
Surface charge:
Electron temperature:
Radiation transport and photoionization:
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University of MichiganInstitute for Plasma Science & Engr.GEC2012
POSITIVE POLARITY Se AND [e]
University of MichiganInstitute for Plasma Science & Engr.
Electron impact ionization source Se, electron density [e], and electric potential contours (spacing = 2 kV)
Plume from primary tube charges the top surface of the transfer channel. Plasma in the transfer channel develops from top to bottom.
Animation SlideGEC2012
POSITIVE POLARITY TRANSFER PROCESS (I)
University of MichiganInstitute for Plasma Science & Engr.
Primary IW front crosses the gap at speed of 7 x 107 cm/s.
IW in primary channel “shorts” out the electric field, translating applied potential to surface of transfer tube with additional charging of surface of transfer tube.
Large E/N in transfer tube ignites the secondary IWs.
Two secondary IWs propagate sideways and gradually fill the whole width of the channel.
The peak electric field is associated with IW front due to the space charge effect.
E-field penetrates the dielectric wall with minor distortion.
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POSITIVE POLARITY TRANSFER PROCESS (II)
University of MichiganInstitute for Plasma Science & Engr.
Initial electron avalanche in the transfer channel starts directly underneath where IW from primary channel intersects.
Transferred avalanche front propagates downwards and sideways.
Electrons inside the transfer channel are heated even before the primary IW front impinges on the top surface.
Electric potential expands following the propagation of the primary/secondary IWs.
The secondary IWs are driven by the same polarity as that of the primary IW.
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POSITIVE POLARITY COMPARISONS
University of MichiganInstitute for Plasma Science & Engr.
Contours of time integrated Ne* density in the simulation show a similar shape to the plasma emission image in the experiments.
Positive plasma transfer is thus a top-down process and the secondary IWs preserve the polarity of the primary IW.
Time integrated Ne* density Plasma emission in experiments (University of Michigan) (GREMI)
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NEGATIVE POLARITY Se AND POTENTIAL
University of MichiganInstitute for Plasma Science & Engr.
Electrons are deposited by the primary IW on the top transfer channel wall. Plasma inside the transfer channel develops from bottom to top. Positive electric potential emerges in the transfer channel.
GEC2012 Animation Slide
NEGATIVE POLARITY [e], AND POTENTIAL
University of MichiganInstitute for Plasma Science & Engr.
A positive IW emerges from the bottom of the transfer tube and impinges upon the top wall.
A positive charge layer forms underneath the top transfer channel wall, turning the negative potential (dash line) into positive potential (solid line).
GEC2012 Animation Slide
NEGATIVE POLARITY TRANSFER PROCESS
University of MichiganInstitute for Plasma Science & Engr.
Initial electron avalanche in the transfer channel starts from the bottom wall.
A positive IW front propagates upwards and then impinges on the top wall.
The impingement of the positive IW front forms a strong positive charge layer on the top inner surface.
The space charge layer generates positive potential inside the transfer channel.
The secondary IWs are driven by the potential with a reversed polarity of the primary IW.
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NEGATIVE POLARITY COMPARISONS
University of MichiganInstitute for Plasma Science & Engr.
Both simulations and experiments show the existence of an intensive plasma layer underneath the inner top wall.
Negative plasma transfer is thus a bottom-up process and the secondary IWs reverse the polarity of the primary IW.
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Time integrated Ne* density Plasma emission in experiments (University of Michigan) (GREMI)
EFFECTS OF PULSE RISE-TIME
University of MichiganInstitute for Plasma Science & Engr.
Negative IWs are more sensitive to the pulse rise time than positive IWs . Increasing pulse rise-time slows down both primary and secondary IWs. For a negative primary IW, a threshold in its rise-time exists beyond which
secondary IWs can not be generated.
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CONCLUDING REMARKS
University of MichiganInstitute for Plasma Science & Engr.
Experiments demonstrate atmospheric pressure plasma transfer by the impingement of a plasma jet produced in a source tube onto the outer surface of a transfer tube which is electrodeless and not connected electronically to the source tube.
For positive polarity, plasma transfer is facilitated by a direct penetration of the electric field through the tube wall. For negative polarity, it is characterized by the formation of a thin space charge layer inside the transfer tube.
Two dimensional numerical modeling with two channels demonstrates that for a positive primary IW, the secondary IWs are produced in a top-down process and preserve the polarity of the primary IW.
For a negative primary IW, the secondary IWs are produced in a bottom-up process and reverse the polarity of the primary IW.
Longer rise-time of the voltage pulse induces a slowing down of both primary and secondary IWs. For a negative primary IW, there is a threshold risetime beyond which secondary IWs can not be generated.
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