We consider here the gravitational collapse of a spherically symmetric inhomogeneous dust cloud described by the Tolman-Bondi models. By studying a general class of these models, we find that the end state of the collapse is either a black hole or a naked singularity, depending on the parameters of the initial density distribution, which are ρc, the initial central density of the massive body, and R₀, the initial boundary. The collapse ends in a black hole if the dimensionless quantity {β} constructed out of this initial data is greater than 0.0113, and it ends in a naked singularity if {β} is less than this number. A simple interpretation of this result can be given in terms of the strength of the gravitational potential at the starting epoch of the collapse.
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Joshi et al. (1995) studied this question.
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