Up: The Kolmogorov turbulence theory
Previous: Acknowledgment
- 1
- A.N.Kolmogorov. Compt Rend. Acod. Sci. U.R.S.S.
30, 301 (1941) ; 32, 16 (1941)
- 2
- S. Tsugé, e-print archive, chao-dyn/9803013(1998)
- 3
- Th.von Kármán and L. Howarth,
Proc.Roy.Soc.London,164A,192(1938)
- 4
- S. Tsugé, Phys.Fluids, 17,22(1974)
- 5
- H.P. Robertson,Proc.Cambr.Phil.Soc,36,209(1940)
- 6
- M. Tanahashi, T. Miyauchi and J. Ikeda, IUTAM Symposium on Simulation, Identification and Organized Stuructures in Flows(ed.J.N.Sorensen et al, Kluwer Acad.Pub.,1999)p.131
- 7
- National Geographic,159,2(1981)
- 8
- M.Tanahashi, private communication (2002)
FIGURE CAPTIONS
Figure 1. Pseudo-singularity formed by a pair of dipoles in the inertial
subrange of the eddy space. The shaded part represents the dissipation
region.[See Eq.(63).]
Figure 2. Evolution of turbulent vortices visualized by a gigantic
turbulent jet : Volcano eruption of Mt. Saint Helens[7].
Figure 3. 1D power spectrum
plotted against 1D wave number
with slenderness ratio
as the parameter. The calculated
spectrum is averaged over five neighboring points to make the comparison
with -5/3 or -2 power laws easier.