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Cylindrical prominences and the magnetic influence of the photospheric boundary

โœ Scribed by I. Lerche; B. C. Low


Publisher
Springer
Year
1980
Tongue
English
Weight
911 KB
Volume
66
Category
Article
ISSN
0038-0938

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โœฆ Synopsis


We construct exact, non-linear, solutions for an horizontal, cylindrical, current-carrying, prominence supported against solar gravity by the action of a Lorentz force. The solutions incorporate the photosphere boundary condition, proposed by van Tend and Kuperus (1978), and analyzed by them for line filaments. Our solutions have finite radius for the prominence material and, as well as satisfying the equations of magnetostatic equilibrium, they allow for the continuity of gas pressure, and of the normal and tangential components of magnetic field across the circular prominence boundary. We show that an infinity of solutions is possible and we illustrate the basic behavior by investigation of a special case.

We also give a prescription for constructing equilibrium fields for any horizontal prominence with arbitrary cross-section and with an arbitrary external magnetic field. The prescription is ideally suited for numerical codes and we suggest that both the equilibrium of such shapes can easily be accomplished numerically together with their evolutionary history. * In doing preliminary calculations prior to this paper, we at one stage computed the energy of a circular cylinder of current. In so doing we had to make use of several integrals recorded by Gradshteyn and Ryzhik (1965). It turned out that two of the recorded integrals are in error and we report here the corrections. On p. 568, 4.317, integral (3) a factor 'In' should be inserted after ~r cot(t); on p. 538, 4.253 integral (4), the upper limit should be ~, not unity.


๐Ÿ“œ SIMILAR VOLUMES


Comparison of the mean photospheric magn
โœ A. Severny; J. M. Wilcox; P. H. Scherrer; D. S. Colburn ๐Ÿ“‚ Article ๐Ÿ“… 1970 ๐Ÿ› Springer ๐ŸŒ English โš– 977 KB

The mean photospheric magnetic field of the sun seen as a star has been compared with the interplanetary magnetic field observed with spacecraft near the earth. Each change in polarity of the mean solar field is followed about 4 89 days later by a change in polarity of the interplanetary field (sect