65th Annual Gaseous Electronics Conference
Volume 57, Number 8
Monday–Friday, October 22–26, 2012;
Austin, Texas
Session RR3: Plasma Propulsion II
1:30 PM–3:00 PM,
Thursday, October 25, 2012
Room: Classroom 202
Chair: John Foster, University of Michigan
Abstract ID: BAPS.2012.GEC.RR3.1
Abstract: RR3.00001 : Rotating spoke phenomena in low pressure E $\times $ B discharges*
1:30 PM–2:00 PM
Preview Abstract
Abstract
Author:
Yevgeny Raitses
(Princeton Plasma Physics Laboratory, Princeton, NJ 08543)
The rotating spoke is azimuthal plasma non-uniformity which has been observed in a variety of low pressure cross-field discharges of cylindrical geometry [1-3]. The spoke can appear in different modes ranging from m=1 to
higher order modes which propagate in the direction perpendicular to electric and magnetic fields with velocities of much lower than E$\times $B velocity [2,3]. Although spoke phenomena is known for more than four
decades, physical mechanism responsible for triggering of the spoke is still not understood. Recent studies of Hall thrusters and Penning-type magnetized plasma discharges demonstrated that the spoke is directly responsible for
the enhancement of the electron cross-field transport in these devices [1,4]. A combination of time-resolving plasma measurements, including high speed imaging and probes suggest that for partially ionized magnetized plasma discharges, the spoke instability is triggered by ionization mechanism [4]. These experimental results are supported by recent
particle-in-cell simulations. The advancement in understanding of the spoke mechanism enabled us to develop and demonstrate effective methods of spoke control, including mode, velocity and direction of the spoke, and spoke
suppression [5]. Among practical implications of these results is the ability to develop more effective methods of plasma confinement and uniformity for magnetically-enhanced discharges and more efficient magnetized plasma thrusters. In collaboration with M. Griswold, L. Ellison, N. J. Fisch, K. Matyash, R. Schneider and A. Smolyakov.\\[4pt]
[1] S. Jaeger, Th. Pierre, C. Rebont, Phys. Plasmas 16, 022304 (2009)\\[0pt]
[2] J. B. Parker, Y. Raitses, N. J. Fisch, Appl. Phys. Lett. 97, 091501 (2010)\\[0pt]
[3] M. S. McDonald, A. D. Gallimore, IEEE Trans. Plasma Sci. 39, 2952 (2011)\\[0pt]
[4] C. L. Ellison, Y. Raitses, N. J. Fisch, Phys. Plasmas 19, 013503 (2012)\\[0pt]
[5] M. E. Griswold, C. L. Ellison, Y. Raitses, N. J. Fisch, Phys. Plasmas 19, 053506 (2012).
*This work was supported by the US DOE under Contract Number DE-AC02-09CH11466
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.GEC.RR3.1