Experimental realization of nearly steady-state toroidal electron plasmasa
Electron plasmas with densities of 5 × 10 6 cm − 3 are trapped in the Lawrence Non-neutral Torus II (LNT II) for times exceeding 1 s. LNT II is a high aspect ratio ( R 0 / a ≳ 10 ) partially toroidal trap (270° arc, B 0 = 670 G ). The m = 1 diocotron mode is launched and detected using isolated...
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Veröffentlicht in: | Physics of plasmas 2009-05, Vol.16 (5) |
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Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Electron plasmas with densities of
5
×
10
6
cm
−
3
are trapped in the Lawrence Non-neutral Torus II (LNT II) for times exceeding 1 s. LNT II is a high aspect ratio
(
R
0
/
a
≳
10
)
partially toroidal trap (270° arc,
B
0
=
670
G
). The
m
=
1
diocotron mode is launched and detected using isolated segments of a fully sectored conducting boundary and its frequency is used to determine the total trapped charge as a function of time. The observed confinement time
(
≈
3
s
)
approaches the theoretical limit
(
≈
6
s
)
set by the magnetic pumping transport mechanism of Crooks and O’Neil [Phys. Plasmas
3, 2533 (1996)]. We also present equilibrium modeling and numerical simulations of the toroidal
m
=
1
mode constrained by experimental data. Future work includes the identification of the dominant transport mechanisms via confinement scaling experiments and measurement of the
m
=
2
mode frequency and development of a strategy for making a transition to fully toroidal confinement. |
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ISSN: | 1070-664X 1089-7674 |
DOI: | 10.1063/1.3118624 |