CLIMATE/EARTH 401�Geophysical Fluid Dynamics�Dynamical Meteorology
Scale analysis: Time scale
Time scales
Time scales
Two coordinate systems
y
z
z’ axis is the same as z, and there is rotation of the x’ and y’ axis
z’
y’
x’
x
Tangential coordinate system
Ω
R
Earth
Place a coordinate system on the surface.
x = west to east (longitude)
y = south to north(latitude)
z = local vertical
Φ
a
The component of the angular velocity in the local vertical.
Coriolis parameter is time scale of rotation
f = 2Ωsin(φ)
at 45°latitude
f0 ~ 10-4 sec-1
Time scales
Time scales
Time scales
Quantitative Comparison
Quantitative Comparison
To make a comparison like this form a ratio and ask how that ratio compares to the number one.
Large scale
If the Rossby number is comparable to or smaller than 1, then rotation is important and we say that the flow is “large-scale.”
Typical numbers
In atmosphere a typical velocity above the ground might be 20 m/sec.
The distance from the peak to a trough of a mid-latitude wave might be 1000 km.
The angular velocity is 7.3 x 10-5 / sec.
A representative velocity of the oceanic Gulf Stream might be 100 cm/sec, what is the length scale that would mean that rotation is important?
A baseball pitcher throws the ball about 90 feet at about 90 miles / hour, is rotation important?
For atmospheric example order 1/7.
For oceanic example order 100/(2*7.3x10-5 L) ~ 1.
Velocity and distance tell us something about time
distance = rate x time
Estimate time as distance/(some average rate)
L ≡ some characteristic distance
U ≡ some characteristic speed
Characteristic time ≡ L/U
Therefore, for acceleration
D ( )/Dt can be characterized by 1/(L/U)
End: Scale analysis: Time scale