62nd Annual Gaseous Electronics Conference
Volume 54, Number 12
Tuesday–Friday, October 20–23, 2009;
Saratoga Springs, New York
Session DM: Kinetics Workshop: Electron Kinetics
4:00 PM–5:30 PM,
Monday, October 19, 2009
Saratoga Hilton
Room: Ballroom 1
Chair: Laxminarajan Raja, University of Texas at Austin
Abstract ID: BAPS.2009.GEC.DM.3
Abstract: DM.00003 : Kinetic Theory of Instability-Enhanced Collisional Effects*
5:00 PM–5:30 PM
Preview Abstract
Abstract
Author:
Scott Baalrud
(University of Wisconsin-Madison)
A generalization of the Lenard-Balescu collision operator is
derived which accounts for the scattering of particles by
instability amplified fluctuations that originate from the
thermal motion of discrete particles (in contrast to evoking a
fluctuation level externally, as is done in quasilinear kinetic
theory) [1]. Emphasis is placed on plasmas with convective
instabilities. It is shown that an instability-enhanced
collective response results which can be the primary mechanism
for scattering particles, being orders of magnitude more frequent
than conventional Coulomb collisions, even though the
fluctuations are in a linear growth phase. The resulting
collision operator is shown to obey conservation laws (energy,
momentum, and density), Galilean invariance, and the Boltzmann
${\mathcal{H}}$-theorem. It has the property that Maxwellian is
the unique equilibrium distribution function; again in contrast
to weak turbulence or quasilinear theories. Instability-enhanced
collisional effects can dominate the physics of low-temperature
plasmas. For example, this theory has been applied to two
outstanding problems: Langmuir's paradox [2] and determining
Bohm's criterion for plasmas with multiple ion species.
Langmuir's paradox is a measurement of anomalous electron
scattering rapidly establishing a Maxwellian distribution in gas
discharges with low temperature and pressure. This may be
explained by instability-enhanced scattering in the
plasma-boundary transition region (presheath) where convective
ion-acoustic instabilities are excited. Bohm's criterion for
multiple ion species is a single condition that the ion fluid
speeds must obey at the sheath edge; but it is insufficient to
determine the speed of individual species. It is shown that an
instability-enhanced collisional friction, due to streaming
instabilities in the presheath, determines this criterion.\\[4pt]
[1] S.D. Baalrud, J.D. Callen, and C.C. Hegna, Phys. Plasmas {\bf
15}, 092111 (2008).\\[0pt]
[2] S.D. Baalrud, J.D. Callen, and C.C. Hegna, Phys. Rev. Lett.
(to appear June 2009); preprint UW-CPTC 09-4 at www.cptc.wisc.edu.
*This material is based upon work supported under a NSF Graduate Research Fellowship and by U.S. DoE Grant No. DE-FG02-86ER53218.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2009.GEC.DM.3