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Boundar Layer Meteorology Lecture 2 Review chapter 1 of Garratt Terminology and Notation Review Some non-dimensional numbers Reynolds Averaging.

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Presentation on theme: "Boundar Layer Meteorology Lecture 2 Review chapter 1 of Garratt Terminology and Notation Review Some non-dimensional numbers Reynolds Averaging."— Presentation transcript:

1 Boundar Layer Meteorology Lecture 2 Review chapter 1 of Garratt Terminology and Notation Review Some non-dimensional numbers Reynolds Averaging

2 Review chapter 1 of Garratt Inner and outer layers (what’s with this, is the outer layer really part of the boundary layer?) Seasonal and geographic variations of the boundary layer’s character.

3 Modeled Boundary Layer Depth

4

5 Observed Boundary Layer Depth

6 Terminology Boundary Layer Regions: Surface Layer Mixed Layer Residual Layer Stable (Nocturnal Boundary) Layer Entrainment Zone Ekman Layer (Outer Layer) Surface Layer

7 Boundary Layer Regions

8 Notation Variables: T, T v, ,  v, , q, x, y, z, Viscosity:  =  du/dy  ;  T  kg/(m s)=Pa/s  –Kinetmatic viscosity:  m 2 /s Summation (Einstein) notation: see Stull handout (pp. 57- 74). Note definitions of the Kronecker delta (and distinction between it and the unit vector), and the alternating unit tensor (Levi-Civita symbol) used to express the cross product.

9 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!). Richardson numbers: ratio of –Flux –Gradient: Ri = (g/  d  dz)/(du/dz) 2 –Bulk

10 Reynolds averaging and Reynolds Stresses t 1 should be enough larger than t 2 so that the average is independent of time.

11 Reynolds averaging and Reynolds Stresses

12 Understanding Reynolds Stress


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