Landau–Hopf theory of turbulence

From Wikipedia, the free encyclopedia
Jump to: navigation, search

In physics, the Landau-Hopf theory of turbulence, named for Lev Landau and Eberhard Hopf, was until the mid 1970s the accepted theory of how a fluid flow becomes turbulent. The theory says that as a fluid flows faster, it develops more and more Fourier modes. At first a few modes dominate, but under stronger forcing the modes become power-law distributed, as in Kolmogorov's theory of turbulence.

[edit] References

Personal tools
Namespaces

Variants
Actions
Navigation
Interaction
Toolbox
Print/export