Anisotropic spectra in two-dimensional turbulence on the surface of a rotating sphere

2001 ◽  
Vol 13 (1) ◽  
pp. 225-240 ◽  
Author(s):  
Huei-Ping Huang ◽  
Boris Galperin ◽  
Semion Sukoriansky
2007 ◽  
Vol 39 (1-3) ◽  
pp. 209-220 ◽  
Author(s):  
Shin-Ichi Takehiro ◽  
Michio Yamada ◽  
Yoshi-Yuki Hayashi

2010 ◽  
Vol 22 (5) ◽  
pp. 056601 ◽  
Author(s):  
Kiori Obuse ◽  
Shin-ichi Takehiro ◽  
Michio Yamada

1997 ◽  
Vol 9 (12) ◽  
pp. 3834-3842 ◽  
Author(s):  
Toru Nozawa ◽  
Shigeo Yoden

1987 ◽  
Vol 184 ◽  
pp. 289-302 ◽  
Author(s):  
Theodore G. Shepherd

It is shown that, for a sufficiently large value of β, two-dimensional flow on a doubly-periodic beta-plane cannot be ergodic (phase-space filling) on the phase-space surface of constant energy and enstrophy. A corresponding result holds for flow on the surface of a rotating sphere, for a sufficiently rapid rotation rate Ω. This implies that the higher-order, non-quadratic invariants are exerting a significant influence on the statistical evolution of the flow. The proof relies on the existence of a finite-amplitude Liapunov stability theorem for zonally symmetric basic states with a non-vanishing absolute-vorticity gradient. When the domain size is much larger than the size of a typical eddy, then a sufficient condition for non-ergodicity is that the wave steepness ε < 1, where ε = 2√2Z/βU in the planar case and $\epsilon = 2^{\frac{1}{4}} a^{\frac{5}{2}}Z^{\frac{7}{4}}/\Omega U^{\frac{5}{2}}$ in the spherical case, and where Z is the enstrophy, U the r.m.s. velocity, and a the radius of the sphere. This result may help to explain why numerical simulations of unforced beta-plane turbulence (in which ε decreases in time) seem to evolve into a non-ergodic regime at large scales.


2007 ◽  
Vol 64 (12) ◽  
pp. 4246-4269 ◽  
Author(s):  
Yoshi-Yuki Hayashi ◽  
Seiya Nishizawa ◽  
Shin-ichi Takehiro ◽  
Michio Yamada ◽  
Keiichi Ishioka ◽  
...  

Abstract Jet formation in decaying two-dimensional turbulence on a rotating sphere is reviewed from the viewpoint of Rossby waves. A series of calculations are performed to confirm the behavior of zonal mean flow generation on the parameter space of the rotation rate Ω and Froude number Fr. When the flow is nondivergent and Ω is large, intense easterly circumpolar jets tend to emerge in addition to the appearance of a banded structure of zonal mean flows with alternating flow directions. When the system allows surface elevation, circumpolar jets disappear and an equatorial easterly jet emerges with increasing Fr. The appearance of the intense easterly jets can be understood by the angular-momentum transport associated with the generation, propagation, and absorption of Rossby waves. When the flow is nondivergent, long Rossby waves tend to be absorbed near the poles. In contrast, when Fr is large, Rossby waves can hardly propagate poleward and tend to be absorbed near the equator.


Author(s):  
Shigeo Yoden ◽  
Keiichi Ishioka ◽  
Michio Yamada ◽  
Yoshi-Yuki Hayashi

Sign in / Sign up

Export Citation Format

Share Document