Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence
Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence
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In our eReader you can find the full English version of the book. Read Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence
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To quickly assess the difficulty of the text, read a short excerpt:
U) become identical with each other, and with (6. 12), It may be verified that if (7. 3), (7. U) are satisfied, then (li. 6) is satisfied by the perturbation theory moments.
At first sight it might be thought that the system (7. 3)> (7. U) does not constitute a much more difficult problem than (6. 12), aside from the increase in the number of unknowns by a factor of two. Actually, the difference in complexity is profound. Equations (7. 3) » (7. Ii) cannot be solved by straightforward step-by- s...tep integration, starting with gLQ(*^)» ^oa^^^* ^^ *^® first place the depend- ence of R_„(0) on a is one of the answers we seek, and, moreover, the right sides of (7. 3) » (7. M even for small z depend on g and R for all argument values. The increase in complexity is not surprising when we consider that the equilibrium nondissipative problem could have been solved in elementary fashion by expanding R (Ti) as a Taylor series about z " 0, expressing the derivatives in terms of simultaneous averages by repeated use of the equations of motion, and averaging over the time-invariant simultaneous distribution.
What to read after Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence?
You can find similar books in the "Read Also" column, or choose other free books by R H Kraichnan to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
U) become identical with each other, and with (6. 12), It may be verified that if (7. 3), (7. U) are satisfied, then (li. 6) is satisfied by the perturbation theory moments.
At first sight it might be thought that the system (7. 3)> (7. U) does not constitute a much more difficult problem than (6. 12), aside from the increase in the number of unknowns by a factor of two. Actually, the difference in complexity is profound. Equations (7. 3) » (7. Ii) cannot be solved by straightforward step-by- s...tep integration, starting with gLQ(*^)» ^oa^^^* ^^ *^® first place the depend- ence of R_„(0) on a is one of the answers we seek, and, moreover, the right sides of (7. 3) » (7. M even for small z depend on g and R for all argument values. The increase in complexity is not surprising when we consider that the equilibrium nondissipative problem could have been solved in elementary fashion by expanding R (Ti) as a Taylor series about z " 0, expressing the derivatives in terms of simultaneous averages by repeated use of the equations of motion, and averaging over the time-invariant simultaneous distribution.
What to read after Statistical Mechanics of Stationary Homogeneous Hydromagnetic Turbulence?
You can find similar books in the "Read Also" column, or choose other free books by R H Kraichnan to read onlineMoreLess
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