Boundary Layer Meteorology Lecture 3 - PowerPoint PPT Presentation

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Boundary Layer Meteorology Lecture 3

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Reynolds averaging and Reynolds Stresses. Review chapter 2 of Garratt ... t1 should be enough larger than t2 so that the average is independent of time. ... – PowerPoint PPT presentation

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Title: Boundary Layer Meteorology Lecture 3


1
Boundary Layer Meteorology Lecture 3
  • Review summation (Einstein) notation
  • Introduce some Non-Dimensional Numbers
  • Reynolds averaging and Reynolds Stresses
  • Review chapter 2 of Garratt

2
Summation (Einstein) notation
3
Some Non-Dimensional Numbers
  • Reynolds number Re VL/?
  • Reynolds number is ratio of acceleration (or
    inertial force) to friction force. It governs
    transition to turbulence (at high Reynolds
    numbers , e.g. about 2300 for pipes highly
    variable, depending on shape of the flow!).
  • For more detail, see http//physics.mercer.edu/hp
    age/friction/ajp/reynolds.html
  • Richardson numbers ratio of buoyant production
    (or destruction) to shear production of
    turbulence.
  • Flux Rf (g/?v)w?/(uw du/dz vw dv/dz)
  • Gradient Ri (g/???d??dz)/(du/dz)2
  • Bulk RiB (g/?v)z(?v-??)/(u2v2)

4
Reynolds averaging and Reynolds Stresses
t1 should be enough larger than t2 so that the
average is independent of time.
5
Reynolds averaging and Reynolds Stresses
6
Understanding Reynolds Stress
Random fluctuations will always tend to remove
local maxima or minima, since, for a maximum they
carry with them momentum from elsewhere, which
must be smaller than the momentum at the maximum.
Similarly, they will tend to remove curvature.
7
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