![]() | ![]() |
Astron. Astrophys. 342, L1-L4 (1999) 5. A new analysis of the Tunguska eventBy means of Eq. (6) we can replace Table 1 with a new table for the breakup speeds of different types of cosmic body (see Table 2). Note that now the inferred speed for an iron body would be too high, and stony bodies provide the most plausible solution. This is consistent with the results of a detailed analysis of several hundreds meteors carried out by Ceplecha & McCrosky (1976) and Ceplecha (1994), who found that a height around 10 km is fairly typical for stony objects. Table 2. Speed of the Tunguska cosmic body vs. strength according to Eq. (6) We can now calculate other data for the Tunguska event solving the
equations of motion and the luminosity equation, according to the
procedure described in Foschini (1998). The results are summarized in
Table 3. The following assumptions have been made: (i) the
luminous efficiency Table 3. Summary on the properties of the Tunguska Cosmic Body a From Ben-Menahem (1975). b Over the horizon. c Clockwise from North. Comparing these results to previous ones and to the available data
(for a review see Vasilyev 1998), we note a generally good agreement,
except for the trajectory inclination over the horizon. The value
obtained here is about Among the authors quoted by Vasilyev, only Sekanina derived an
angle lower than ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1999 Online publication: December 22, 1998 ![]() |