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  1. Elftrytub
  2. These modes of behavior may all be observed in the familiar rotating-basin experiments, described by Fultz, et al. (1959) and Hide (1958).
  3. Certain hydrodynamical systems exhibit steady-state flow patterns, while others oscillate in a regular periodic fashion.
  4. Thus we shall be involved with the ultimate behavior of the solutions, as opposed to the transient behavior associated with arbitrary init
  5. 8
  6. Ordinarily, however, nonperiodic solutions cannot readily be determined except by numerical procedures.
  7. Under certain conditions the resulting flow is as symmetric and steady as the heating which gives rise to it.
  8. Thus we shall be involved with the ultimate behavior of the solutions, as opposed to the transient behavior associated with arbitrary init
  9. Such procedures involve replacing the continuous variables by a new finite set of functions of time, which may perhaps be the values of the
  10. It is sometimes possible to obtain particular solutions of these equations analytically, especially when the solutions are periodic or in
  11. Because instantaneous turbulent flow patterns are so irregular, attention is often confined to the statistics of turbulence, which, in con
  12. Under certain conditions the resulting flow is as symmetric and steady as the heating which gives rise to it.
  13. Ordinarily, however, nonperiodic solutions cannot readily be determined except by numerical procedures.
  14. For certain purposes many systems may be treated as conservative systems, in which the total energy, or some other quantity, does not vary
  15. Lack of periodicity is very common in natural systems, and is one of the distinguishing features of turbulent flow.
  16. Because instantaneous turbulent flow patterns are so irregular, attention is often confined to the statistics of turbulence, which, in con
  17. Ordinarily, however, nonperiodic solutions cannot readily be determined except by numerical procedures.
  18. Such procedures involve replacing the continuous variables by a new finite set of functions of time, which may perhaps be the values of the
  19. In this study we shall work with systems of deterministic equations which are idealizations of hydrodynamical systems.
  20. Under certain conditions the resulting flow is as symmetric and steady as the heating which gives rise to it.