Geophysical research has focused on flows, such as ocean currents, as two dimensional. Two dimensional point or blob vortex models have the advantage of having a Hamiltonian, whereas 3D vortex filament or tube systems do not necessarily have one, although they do have action functionals. On the other hand, certain classes of 3D vortex models called nearly parallel vortex filament models do have a Hamiltonian and are more accurate descriptions of geophysical and atmospheric flows than purely 2D models, especially at smaller scales. In these quasi-2D'' models we replace 2D point vortices with vortex filaments that are very straight and nearly parallel but have Brownian variations along their lengths due to local self-induction. When very straight, quasi-2D filaments are expected to have virtually the same planar density distributions as 2D models. An open problem is when quasi-2D model statistics behave differently than those of the related 2D system and how this difference is manifested. In this paper we study the nearly parallel vortex filament model of Klein, Majda, Damodaran in statistical equilibrium. We are able to obtain a free-energy functional for the system in a non-extensive thermodynamic limit that is a function of the mean square vortex position @math and solve for @math . Such an explicit formula has never been obtained for a non-2D model. We compare the results of our formula to a 2-D formula of Lim:2005 and show qualitatively different behavior even when we disallow vortex braiding. We further confirm our results using Path Integral Monte Carlo (Ceperley (1995)) permutations and that the Klein, Majda, Damodaran model's asymptotic assumptions for parameters where these deviations occur.
@cite_12 has done some excellent simulations of vortex tangles in He-4 with rotation, boundary walls, and vortex reconnections to study disorder in rotating superfluid turbulence. Because vortex tangles are extremely curved, they applied the full Biot-Savart law to calculate the motion of the filaments in time. Their study did not include any sort of comparison to 2-D models because for most of the simulation vortices were far too tangled. The inclusion of rigid boundary walls, although correct for the study of He-4, also makes the results only tangentially applicable to the KMD system we use.
@cite_12
2090218426
Almost all studies of vortex states in helium II have been concerned with either ordered vortex arrays or disordered vortex tangles. This work numerically studies what happens in the presence of both rotation (which induces order) and thermal counterflow (which induces disorder). We find a new statistically steady state in which the vortex tangle is polarized along the rotational axis. Our results are used to interpret an instability that was discovered experimentally by [Phys. Rev. Lett. 50, 190 (1983)] and the vortex state beyond the instability that has been unexplained until now.