Rossby Waves (waves in the upper air westerlies).

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Presentation transcript:

Rossby Waves (waves in the upper air westerlies)

Coriolis is easy. The spin about a vertical axis is the greatest at the poles. It is zero at the Equator. Can you see why? To describe turn about the vertical axis, use f = 2  sin  How is this guy going to turn? How about this guy? Doesn’t he turn?

To see relative vorticity, it helps to actually calculate some: What is the Relative Vorticity (  ) at KNYX? With winds like these, what kind of vorticity do you have? Your choices are: Cyclonic (+) or Anticyclonic (-)

Reminders :  ~  v/  x -  u/  y 1 knot = m s km = 4 x 10 5 m So,  = (56.6 m s -1 /4 x 10 5 m) – (-69.4 m s -1 /4 x 10 5 m) = x s x s -1 = 31.5 x s -1 It’s positive and therefore cyclonic. Didn’t it look cyclonic or counter- clockwise in the Northern Hemisphere?

Now back to Rossby: We assume friction is very small in the upper air. Also, tilting is very small on the synoptic scale (more about that next semester). Rossby also assumed no vertical motion (w = 0). That stifles divergence so D = 0. ` This is called “Conservation of Absolute Vorticity”

Constant absolute vorticity trajectories naturally go in wavelike patterns Conservation of Absolute Vorticity

In addition to the fact that the atmosphere must consist of waves, Rossby used the conservation of Absolute Vorticity to show that the speed of those waves can be calculated. We won’t derive that here. Take Dynamics to see how it works. The Rossby wave equation can help us understand how weather systems move. What is the difference between wave speed (c) and wind speed (U)?

Watch this wave trough The trough finishes here, 1000 nm east and 24 hours later So the trough moves at a speed of 42 nm/hour (knots) but the winds in the trough are much greater than that, up to 95 knots! So, c ~ 42 knots but we can estimate U ~ 70 knots.

We estimated U ~ 70 knots and the wave we looked at was around 45 N. But it’s wavelength is not 3000 miles as the table would suggest. What went wrong?

That means we can fit 3.3 waves of that length around the hemisphere circle.

This is a simple wave 3 simulation. The colors are wind speed. Notice the three blue maxima (jet streams)in the troughs.

Animating …

Real upper air patterns are quite a bit more complex. In this actual hemispheric loop from 2006 the colors represent wind speed with white height contours showing the troughs and ridges. Do you see wave 3? How about wave 2? 8? Which waves are progressive? Why are they progressive?

This is the 300 mb flow over North America at that time.

This is the corresponding surface loop.

Here’s a loop from June, Short waves move into the long wave which stays mostly stationary. Around June 18, an Omega Block forms

This is the surface during June While surface Lows move with the short waves, a tendency for unsettled weather persists under the western trough.

Class assignment As seen on the 300 mb wave loop, the upper air pattern over North America is often one complete wave. Usually there is a ridge over the west and a trough in the eastern half of the nation. That is a pattern that recurs more often than any other. If the wave over North America is centered at 45 º N, what wave number is that? Use the Rossby Wave Equation.