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1. The horizontal equations of motion: smaller-scale motion
2. The vertical equation of motion
3. The thermal wind
ATOC 4720 class34
H L
Northern Hemisphere (NH):
P1 P2 P3 P4 P5x
y
PGFCF
Previous class:GEOSTROPHY:
Geostrophic wind value:
In PBL, friction is important.
Frictional convergence toward the low pressure! Important!
V cross the isobars!
Cross-isobar flow due to friction
The gradient wind
x
y
z
1. Smaller-scale convection: GEOSTROPHY BREAKS DOWN
Observations for small-scale convection:
Velocity U-V: 20 m/s;Time T (100-1000s)= S
Acceleration term:
Coriolis term:
Therefore, the Coriolis term can be NEGLECTED! Geostrophy breaks down!
0
2. The vertical equation of motionIn z direction: Newton’s second law of motion for unit mass:
negligible Free atmospherenegligible
Large-scale motion, T: 1day; W:10m/s:
Even for T=1000s,
Hydrostatic balanceHydrostatic balance is well satisfied even by mesoscale convection.
Exercise: find out for what scale convection (vertical velocity and timescale), hydrostatic balance can break down.
3. Thermal wind relationGeostrophic wind speed:
Perform vertical derivation:
Between 2 layers:
Substitude (Z2-Z1) from the hypsometric equation (2.29)
(for dry air)