Fig. 1
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Illustration of the pancake model presented by Chyba et al. (1993). The fragmentation starts when the ram pressure, P, exceeds the initial bulk strength, S0. And the airburst occurs, or the peak brightness is reached, at the very short moment when the windward radius of the object expands to N times the initial diameter of the object, R0. The height of fragmentation is the altitude where the fragmentation begins, which differs from the height of the airburst or, equivalently, the peak brightness.
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