M. Beckers et al., Dynamics of pancake-like vortices in a stratified fluid: experiments, model and numerical simulations, J FLUID MEC, 433, 2001, pp. 1-27
The dynamics and the three-dimensional structure of vortices in a linearly
stratified, non-rotating fluid are investigated by means of laboratory expe
riments, an analytical model and through numerical simulations. The laborat
ory experiments show that such vortices have a thin pancake-like appearance
, Due to vertical diffusion of momentum the strength of these vortices decr
eases rapidly and their thickness increases in time. Also it is found that
inside a vortex the linear ambient density profile becomes perturbed, resul
ting in a Local steepening of the density gradient. Based on the assumption
of a quasi-two-dimensional axisymmetric how (i.e. with zero vertical veloc
ity) a model is derived from the Boussinesq equations that illustrates that
the velocity field of the vortex decays due to diffusion and that the vort
ex is in so-called cyclostrophic balance. This means that the centrifugal f
orce inside the vortex is balanced by a pressure gradient force that is pro
vided by a perturbation of the density profile in a way that is observed in
the experiments. Numerical simulations are performed, using a finite diffe
rence method ir a cylindrical coordinate system. As an initial condition th
e three-dimensional vorticity and density structure of the vortex, found wi
th the diffusion model, are used. The influence of the Froude number, Schmi
dt number and Reynolds number, as well as the initial thickness of the vort
ex, on the evolution of the flow are investigated. For a specific combinati
on of flow parameters it is found that during the decay of the vortex the r
elaxation of the isopycnals back to their undisturbed positions can result
in a stretching of the vortex. Potential energy of the perturbed isopycnals
is then converted into kinetic energy of the vortex. However, when the str
atification is strong enough (i,e, for small Froude numbers), the evolution
of the vortex call be described almost perfectly by the diffusion model al
one.