Astronomy and Astrophysics – Astrophysics
Scientific paper
Oct 2002
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=2002ap%26ss.282..447c&link_type=abstract
Astrophysics and Space Science, v. 282, Issue 2, p. 447-460 (2002).
Astronomy and Astrophysics
Astrophysics
13
Scientific paper
A mathematical description of the solar wind flow-tube geometry is proposed. The expansion factor of the flow tube f(r) (= a/r 2, r is the heliocentric distance and a is the flow-tube cross-section area)increases monotonically from 1 at the coronal base to m at r c, and approaches its asymptotic value f ∞ nearly in a width of2σ c . The flow tube with f m =f infin is demonstrated to be approximately equivalent to that given by Kopp and Holzer (1976) for the fast solar wind, and it presumably represents slow wind tubes as f m is substantially larger than f ∞. In terms of an Alfvén wave-driven solar wind model, the effect of the flow-tube geometry on solar wind properties is examined. It is found that with the same flow conditions at the coronal base an expansion factor which increases monotonically with the radial distance results in a fast solar wind solution, whereas a flow tube which undergoes an expansion-contraction-reexpansion process creates a slow solar wind solution. Among the four flow-tube parameters the maximum expansion factor f m has the strongest effect, and the associated Laval-nozzle formed by the contraction and reexpansion of theflow tube plays a crucial role in determining solar wind properties. It is suggested that one must take the effect of the flow-tube geometry into account while constructing reasonable flow-tube models for the slow solar wind.
Chen Yafeng
Hu Yong-Qing
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