50th Annual Meeting of the Division of Plasma Physics
Volume 53, Number 14
Monday–Friday, November 17–21, 2008;
Dallas, Texas
Session NI2: Intense Beams, Plasma Filaments, and Nonlinear Waves
9:45 AM–12:45 PM,
Wednesday, November 19, 2008
Room: Landmark B
Chair: Howard Milchberg, University of Maryland
Abstract ID: BAPS.2008.DPP.NI2.2
Abstract: NI2.00002 : Collisionless plasma expansion into vacuum: two new twists on an old problem*
10:15 AM–10:45 AM
Preview Abstract
Abstract
Author:
Alexey Arefiev
(Institute for Fusion Studies, The University of Texas at Austin)
Plasma expansion into vacuum is a generic problem with a broad
range of applications. Of particular interest are those regimes
where the expanding plasma consists of energetic electrons and
cold ions. The expansion is then caused by electron pressure and
serves as an energy transfer mechanism from electrons to ions.
Collisional plasma expansion is similar to the gas-dynamic
expansion, with the fluid description applicable, whereas
collisionless plasma expansion requires a kinetic treatment,
especially for the energetic electrons. The collisionless
expansion is often described under the assumption that the
electron distribution is Maxwellian [1]. However, this assumption
is not universally relevant, since the expansion may lead to a
significant distortion of the electron distribution function.
Also, non-Maxwellian electrons may force the quasineutrality
condition to break down. This talk presents two problems [2,3]
which illustrate the above kinetic effects. The first one is the
problem of a magnetic nozzle that transforms an incoming subsonic
plasma flow into a supersonic jet. The second is the problem of
an expanding nanoplasma (cluster) with a two-component electron
distribution. In the nozzle problem, a magnetic mirror, together
with the expanding plasma boundary, generates a trapped electron
population downstream. This population is decoupled from the
plasma source and, consequently, it undergoes adiabatic cooling.
The resulting distortion of the electron distribution function is
a new element not captured by the usually used Boltzmann
relation. In the cluster problem, the key feature is the initial
two-component electron distribution with a cold majority and a
hot minority both occupying the same volume prior to the
expansion. The cluster problem exhibits a breakdown of
quasineutrality manifested by a double-layer inside the flow.
Both problems are illustrated with closed-form analytical
solutions [2,3]. This work was supported by the US DOE NNSA under
Contract No. DE-FC52-08NA28512 and Ad Astra Rocket Company. [1]
A. V. Gurevich, L. V. Pariiskaya, and L. P. Pitaevskii, Sov.
Phys. JETP 22, 449 (1966). [2] A. V. Arefiev and B. N. Breizman,
Phys. Plasmas 15, 042109 (2008). [3] B. N. Breizman and A. V.
Arefiev, Phys. Plasmas 14, 073105 (2007).
*In collabotation with Boris Breizman, Institute for Fusion Studies, The University of Texas at Austin.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.DPP.NI2.2