A variational principle for surface waves in magnetohydrodynamics
Author:
Bhimsen K. Shivamoggi
Journal:
Quart. Appl. Math. 41 (1983), 31-33
MSC:
Primary 76W05; Secondary 49H05
DOI:
https://doi.org/10.1090/qam/720366
MathSciNet review:
720366
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Abstract: A variational principle for the motion of the interface between an infinitely conducting fluid and a vacuum magnetic field is given. This variational principle not only gives the Laplace equation governing the velocity potential and the magnetic-field potential, but also provides all the boundary conditions appropriate to the interface between an infinitely conducting fluid and a vacuum magnetic field. However, unlike the hydrodynamical case, this variational principle does not have the simple physical interpretation of the stationarity of the fluid pressure + magnetic field pressure.
- H. Bateman, The transformation of partial differential equations, Quart. Appl. Math. 1 (1944), 281–296. MR 9686, DOI https://doi.org/10.1090/S0033-569X-1944-09686-0
L. Debnath, Plasma Phys. 19, 263 (1977)
L. Debnath, Plasma Phys. 20, 343 (1978)
- J. C. Luke, A variational principle for a fluid with a free surface, J. Fluid Mech. 27 (1967), 395–397. MR 210376, DOI https://doi.org/10.1017/S0022112067000412
B. K. Shivamoggi, J. Plasma Phys., 27, 321 (1982)
H. Bateman, Partial differential equations, Cambridge Univ. Press, 1944
L. Debnath, Plasma Phys. 19, 263 (1977)
L. Debnath, Plasma Phys. 20, 343 (1978)
J. C. Luke, J. Fluid Mech. 27, 395 (1967)
B. K. Shivamoggi, J. Plasma Phys., 27, 321 (1982)
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Article copyright:
© Copyright 1983
American Mathematical Society