Abstract
Computational vortex particle method simulations of a perturbed vortex ring are performed to recreate and understand the instability seen in impacting water drop experiments. Three fundamentally different initial vorticity distributions are used to attempt to trigger a Widnall instability, a Rayleigh centrifugal instability, or a vortex breakdown-type instability. Simulations which simply have a perturbed solitary ring result in an instability similar to that seen experimentally. Waviness of the core which would be expected from a Widnall instability is not visible. Adding an opposite-signed secondary vortex ring or an image vortex ring to the initial conditions, to trigger a Rayleigh or breakdown respectively, does not appear to significantly change the instability from what is seen with a solitary ring. This suggests that a Rayleigh or vortex breakdown-type instability are not likely at work, though tests are not conclusive. Perhaps the opposite-signed secondary vortex was not strong enough or placed appropriately. Elliptical streamlines , as expected, are visible in the core of the solitary ring at early times. Support from the Canadian Natural Sciences and Engineering Research Council grant 41747 is gratefully acknowledged.
| Original language | English |
|---|---|
| Article number | Abstract: R6.00005 |
| Journal | American Physical Society. Bulletin |
| Volume | 58 |
| Issue number | 8 |
| ISSN | 0003-0503 |
| Publication status | Published - 2013 |
| Event | 66th Annual Meeting of the American Physical Society Division of Fluid Dynamics - Pittsburgh, PA, United States Duration: 24 Nov 2013 → 26 Nov 2013 Conference number: 66 |
Conference
| Conference | 66th Annual Meeting of the American Physical Society Division of Fluid Dynamics |
|---|---|
| Number | 66 |
| Country/Territory | United States |
| City | Pittsburgh, PA |
| Period | 24/11/2013 → 26/11/2013 |
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