Abstract
A renormalization-group fixed point is found, corresponding to chaotic mixing in the Rayleigh-Taylor instability problem. The outer envelope of the mixing region, adjacent to the heavy fluid, is dominated by a merger of unstable modes (bubbles of light fluid) and dynamically changing length scales. A statistical model is introduced as an approximation to the full two-fluid Euler equation to describe the mixing envelope. Molecular-chaos and continuous-time approximations to this model define an approximate renormalization-group equation, which is shown to have a nontrivial fixed point.
| Original language | English |
|---|---|
| Pages (from-to) | 2137-2139 |
| Number of pages | 3 |
| Journal | Physical Review Letters |
| Volume | 64 |
| Issue number | 18 |
| DOIs | |
| State | Published - 1990 |
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