Vortical and wave modes in 3D rotating stratified flows: random large-scale forcing

Utilizing an eigenfunction decomposition, we study the growth and spectra of energy in the vortical (geostrophic) and wave (ageostrophic) modes of a three-dimensional (3D) rotating stratified fluid as a function of epsilon=f/N, where f is the Coriolis parameter and N is the Brunt-Vaisala frequency. Throughout, we employ a random large-scale forcing in a unit aspect ratio domain and set these parameters such that the Froude and Rossby numbers are roughly comparable and much less than unity. Working in regimes characterized by moderate Burger numbers, i.e. Bu=1/epsilon(2)<1 or Bu >= 1, our results indicate profound change in the character of vortical and wave mode interactions with respect to Bu=1. Indeed, previous analytical work concerning the qualitatively different nature of these interactions has been in limiting conditions of rotation or stratification domination (i.e. when Bu << 1 or Bu >> 1, respectively). As with the reference state of c=1, for c<1 the wave mode energy saturates quite quickly and the ensuing forward cascade continues to act as an efficient means of dissipating ageostrophic energy. Further, these saturated spectra steepen as epsilon decreases: we see a shift from k(-1) to k(-5/3) scaling for k(f)1 the wave mode energy never saturates and comes to dominate the total energy in the system. In fact, in a sense the wave modes behave in an asymmetric manner about epsilon=1. With regard to the vortical modes, for epsilon <= 1, the signatures of 3D quasigeostrophy are clearly evident. Specifically, we see a k(-3) scaling for k(f)1 and increasing, the vortical modes contain a progressively smaller fraction of the total energy indicating that the 3D quasigeostrophic subsystem, though always present, plays an energetically smaller role in the overall dynamics. Combining the vortical and wave modes, the total energy for k>k(f) and epsilon <= 1 shows a transition as k increases wherein the vortical modes contain a large portion of the energy at large scales, while the wave modes dominate at smaller scales. There is no such transition when epsilon>1 and the wave modes dominate the total energy for all k>k(f).