We investigate the collapse of an axisymmetric cavity or bubble inside a fluid of small viscosity, like water. Any effects of the gas inside the cavity as well as of the fluid viscosity are neglected. Using a slender-body description, we compute the local scaling exponent α=dlnh₀/dlnt^' of the minimum radius h₀ of the cavity, where t^' is the time from collapse. The exponent α very slowly approaches a universal value according to α=1/2+1/[4√-ln(t^')]. Thus, as observed in a number of recent experiments, the scaling can easily be interpreted as evidence of a single nontrivial scaling exponent. Our predictions are confirmed by numerical simulations.
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Eggers et al. (2007) studied this question.
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