Section 2: The Planetary Boundary Layer Chapter 5 in “Dynamic Meteorology”
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Transcript of Section 2: The Planetary Boundary Layer Chapter 5 in “Dynamic Meteorology”
Section 2: The Planetary Boundary Layer
Chapter 5 in “Dynamic Meteorology”
DefinitionThe planetary boundary layer is
that portion of the atmosphere in which the flow field is strongly influenced directly by interaction with the surface of the earth.
How does the surface of the earth influence the flow field?
Eddies transport heat, moisture and momentum.The mechanical impact of all subgrid-scale motions upon an observable flow is collectively called a frictional force.
Force Balance
p −2δp
p −δp
p
Top of the PBL At the surfaceWithin the PBL
V
PGF
Co
PGF ~ Co
p −2δp
p −δp
p
PGF
Fr
PGF ~ Fr
p −δp
p
p −2δpPGF
Co
V
Three-way balance
A Tea Cup Experiment
Ekman pumping (or Ekman suction) and Secondary
Circulation
The flow in the free atmosphere is indirectly affected by the friction near the surface through Ekman pumping or Ekman suction.
Mass convergence into low pressure centers and mass divergence out of high pressure centers will eventually destroy the weather systems while forcing upward vertical motion in low and downward vertical motion in high.
Equations in the PBL
Do we have a closed equation set?
No! Closure assumptions must be made to approximate the unknown fluxes in terms of the mean state variables.
Assume horizontal homogeneous…
Assume horizontal homogeneous…
Assume force balance in the PBL…
0
0
Apply the flux-gradient theory
Assume the vertical flux of a given field is proportional to the local gradient of the mean:
€
u 'w ' = −Km(∂ u
∂z)
€
v'w ' = −Km(∂ v
∂z)
€
u 'θ ' = −Kh(∂θ
∂z)
where Km is the eddy viscosity coefficient and Kh is the eddy diffusion of heat.
Assuming Km is a constant, we have:
We will examine the effect of friction on the wind in the Ekman layer:
How does the wind field change with height?
What determines the Ekman pumping (or Ekman suction)?
How is the Ekman layer coupled to the free atmosphere?
LimitationsThe Ekman layer solution does not apply to the
surface layer.
The flux-gradient approximation may not be valid.
Km is not a constant in the PBL.
The atmosphere is not neutral.
Barotropic, neutral atmosphere
Stable Stratification
Spin-down above the PBL
Adiabatic cooling
BL drag + free atmosphere rotation convergence over cyclonic circulation upward mass transport out of the Ekman layer divergence above the Ekman layer spin-down of the cyclone in the free atmosphere
BL drag + free atmosphere rotation convergence over cyclonic circulation Ekman pumping adiabatic cooling (stable stratification) thermal wind balance