Spectral characteristics of two-dimensional turbulent convection in a vertical slot

1988 ◽  
Vol 29 (2) ◽  
pp. 196-200 ◽  
Author(s):  
V. A. Barannikov ◽  
P. G. Frik ◽  
V. G. Shaidurov
2017 ◽  
Vol 29 (11) ◽  
pp. 111102 ◽  
Author(s):  
Andrea Mazzino

1998 ◽  
Vol 59 (2) ◽  
pp. 367-385 ◽  
Author(s):  
A. THYAGARAJA

This paper and a forthcoming one develop the spectral theory of ballooning transformations relevant to tokamak physics from first principles in a rigorous and yet intuitively clear manner. The power of the ballooning representation to throw light on the spectral characteristics of the plasma problems to which it is applicable is emphasized, and examples are given to illustrate the general notions. The ballooning representation is shown to be essentially a method to separate variables and reduce two-dimensional partial differential equations with periodic coefficients to infinite sets of soluble ordinary differential equations. This paper is concerned with an elementary approach to the techniques in the context of nearly exactly soluble problems involving the anisotropic diffusion operator in toroidal geometry. Two different perturbation methods are discussed. Applications to plasma instability problems and the subtleties involving the continuous spectra of ballooning operators will be taken up in Part 2.


2021 ◽  
Author(s):  
Jian-Chao He ◽  
Ming-Wei Fang ◽  
Zhen-Yuan Gao ◽  
Shi-Di Huang ◽  
Yun Bao

1989 ◽  
Vol 207 ◽  
pp. 419-452 ◽  
Author(s):  
E. C. Itsweire ◽  
K. N. Helland

The influence of stabilizing buoyancy forces on the spectral characteristics and spectral energy transfer of grid-generated turbulence was studied in a ten-layer closed-loop stratified water channel. The results are compared to the limiting ideal cases of the three-dimensional turbulence and two-dimensional turbulence theories. The velocity power spectra evolve from a classical isotropic shape to a shape of almost k−2 after the suppression of the net vertical mixing. This final spectral shape is rather different from the k−3 to k−4 predicted by the theory of two-dimensional turbulence and could result from the interaction between small-scale internal waves and quasi-two-dimensional turbulent structures as well as some Doppler shift of advected waves. Several lengthscales are derived from the cospectra of the vertical velocity and density fluctuations and compared with the buoyancy, overturning and viscous lengthscales measured in previous studies, e.g. Stillinger, Helland & Van Atta (1983) and Itsweire, Helland & Van Atta (1986). The smallest turbulent scale, defined when the buoyancy flux goes to zero, can be related to the peak of the cospectra of the buoyancy flux. This new relationship can be used to provide a measure of the smallest turbulent scale in cases where the buoyancy flux never goes to zero, i.e. a growing turbulent stratified shear flow. Finally, the one-dimensional energy transfer term computed from the bispectra shows evidence of a reverse energy cascade from the small scales to the large scales far from the grid where buoyancy forces dominate inertial forces. The observed reverse energy transfer could be produced by the development of quasi-two-dimensional eddies as the original three-dimensional turbulence collapses.


Sign in / Sign up

Export Citation Format

Share Document