DYNAMIC CLASSIFICATION OF BELTRAMI FLOWS

Abstract

We study four configurations of Beltrami flows (BFs) defined as ∇ × v = ±γ ^±v, where γ > 0 is an eigenvalue and which have a progressive rotating wave dynamics (PRWs) that satisfies the dynamic property (DP) [1], which allows us to classify them on the basis of the eigenvalues that result in each configuration. The first configuration corresponds to an infinite volume domain without contours. The classifier eigenvalue is γ ^± _ph = 2/ v_ph± where k is the modulus of the wave vector that forms an angle θ with the rotation axis. The result is a finite-amplitude, transverse, dispersive, circularly polarised, planar PRWs with a continuous spectrum. The second configuration has the same domain as configuration one. The classifying eigenvalue is γ ^± _ph = 2/ v_ph± with v_ph being the phase velocity, with v_ph+ < 0 and v_ph− > 0. They are axi-symmetric or non-axi-symmetric along the axis of rotation, of finite amplitude, non-dispersive and with motion between concentric cylinders at which the radial velocity equals zero. In the third configuration the fluid is confined in an infinite cylinder. The classifying eigenvalue is again γ ^± _ph but it results discretized by the boundary conditions on the cylinder wall. Classification is exemplified for v_ph+ = −0.1 and three rotating modes with m = 0, m = 1 y m = 2. These are finite amplitude dispersive PRWs.  The fourth configuration consists of a rotational-translational flow, characterized by the Rossby number R₀ (=U/a Ω) which is an intake flow to a semi-infinite cylinder. The classifying eigenvalue is γ ^± _ph with v_ph± = ∓R₀. These are PRWs, of the same type as in the infinite cylinder, but dependent on R₀. It is shown that these waves exist only in the interval R₀ ∈ (0,0.642]. Where for R₀ = 0.642 one has only the mode with m = 1 and as R₀ decreases the modes m = 0 and m ≥ 2 arise successively. It is observed that, for the same R₀, waves of the same sign of frequency do not exchange energy. For each configuration the possibilities and conditions of resonant triadic interactions are analyzed.