Alfvén waves, made to propagate along an ambient magnetic field and polarized transverse to a gravitational field g, with wave amplitude stratified along g, are shown to reduce the growth rate of interchange instability by increasing the effective inertia by a factor of 1+(B¯yB¯zkz)2, where B¯z is the ambient magnetic field, kz is the wavenumber, and B¯y is the wave amplitude shear. Appropriately placed Alfvén wave power could thus be used to enhance the stability of interchange and ballooning modes in tokamaks and other interchange-limited magnetically confined plasmas.

1.
B. R.
Suydam
, in
Peaceful Uses of Atomic Energy
,
Proceedings of the 2nd International Conference of the United Nations
(
United Nations
,
Geneva
,
1958
), Vol.
31
, p.
157
.
2.
J. P.
Freidberg
,
Ideal Magnetohydrodynamics
(
Plenum
,
New York
,
1987
).
3.
J.
Wesson
,
Tokamaks
,
Oxford Science Publications
(
Clarendon
,
Oxford
,
1997
).
4.
J. R.
Myra
,
D. A.
D’Ippolito
, and
G. L.
Frances
,
Phys. Fluids
30
,
148
(
1987
).
5.
J. P.
Goedbloed
and
D. A.
D’Ippolito
,
Phys. Fluids B
2
,
2366
(
1990
).
6.
D. A.
D’Ippolito
,
J. R.
Myra
,
S. C.
Jardin
,
M. S.
Chance
, and
J.
Valeo
,
Phys. Plasmas
2
,
3249
(
1995
).
7.
R.
White
,
D.
Monticello
,
M. N.
Rosenbluth
,
H.
Strauss
, and
B. B.
Kadomtsev
, in
Plasma Physics and Controlled Nuclear Fusion Research
(
International Atomic Energy Agency
,
Vienna
,
1975
), paper CN-33/A 13-3.
8.
H. R.
Strauss
,
Phys. Fluids
19
,
134
(
1976
).
9.
K. V.
Roberts
and
J. B.
Taylor
,
Phys. Rev. Lett.
8
,
197
(
1962
).
10.
A. B.
Hassam
,
Phys. Fluids B
4
,
485
(
1992
).
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