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| | Introduction |
 | | The typical temperatures of the first, so-called standard accretion disc model are hot enough (see Frank, King and Raine 1985 [6] for equations describing the structure of the standard disc) to ensure a very high degree of ionisation. |
 | | This notwithstanding, nonviscous discs, with dynamics dominated by angular momentum removal via centrifugally driven winds, are conceivable, and models of such discs have been constructed (Königl 1989 [8], Lovelace, Romanova and Newman 1994 [11], Li 1995 [10]). |
 | | The space is divided into two regions, the inside of the disc and the outside of the disc, by the disc's surface defined to coincide with its halfthickness. |
| www.lpi.usra.edu /science/tom/mn/node1.html (1225 words) |
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