Abstract
The appearance of a singularity in the velocity-field vorticity ω at an isolated point irrespective of the symmetry of initial distribution is demonstrated numerically. The behavior of maximal vorticity |ω| near the collapse point is well approximated by the dependence (t 0−t)−1, where t 0 is the collapse time. This is consistent with the interpretation of collapse as the breaking of vortex lines.
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Translated from Pis’ma v Zhurnal Éksperimental’no\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l}\) i Teoretichesko\(\overset{\lower0.5em\hbox{$\smash{\scriptscriptstyle\smile}$}}{l}\) Fiziki, Vol. 74, No. 7, 2001, pp. 402–406.
Original Russian Text Copyright © 2001 by Zheligovsky Kuznetsov, Podvigina.