possible type of initial singularity other than that of the big bang would be the singularity in a white hole – which, as we recall from Chapter 7, is the time-reverse of a black hole (refer back to Fig. 7.14). But we have seen that the singularities inside black holes satisfy WEYL → ∞, so for a white hole, also, we must have WEYL → ∞. But the singularity is now an initial singularity, for which WCH requires WEYL = 0. Thus WCH rules out the occurrence of white holes in our universe! (Fortunately, this is not only desirable on thermodynamic grounds – for white holes would violently disobey the
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