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Middle-Latitude Cyclones - II

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Title: Slide 1 Author: Konstantin Matchev Last modified by: Katia Matcheva Created Date: 8/23/2005 2:54:26 PM Document presentation format: On-screen Show – PowerPoint PPT presentation

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Title: Middle-Latitude Cyclones - II


1
Middle-Latitude Cyclones - II
2
Review and Outline
  • The polar front model (Norwegian model) of a
    developing mid-latitude cyclonic storm represents
    a simplified but useful model of how an ideal
    storm progresses through the stages of birth,
    maturity and dissipation.
  • Cyclogenesis, lee-side lows, northeasters, bombs.
  • For a surface mid-latitude cyclonic storm to
    form, there must be an area of upper-level
    divergence above the surface low. For the surface
    storm to intensify, this region of upper level
    divergence must be greater than surface
    convergence.
  • When the polar-front jet stream develops into a
    looping wave, it provides an area of upper-level
    divergence for the development of surface
    mid-latitude cyclonic storms.
  • The curving nature of the polar-front jet stream
    tends to direct surface mid-latitude cyclonic
    storms northeastward and surface anticyclones
    southeastward.
  • Skip the sections on Vorticity, Divergence, and
    Developing Mid-Latitude Cyclones and Polar
    Lows

3
The life of a mid-latitude (wave) cyclone
4
(No Transcript)
5
Satellite image from Chapter 1 Fig. 1.13.
6
What happens with the high and low pressure
centers over time?
  • The development of a cyclonic wave is determined
    by the motion of the air aloft
  • the air flow aloft is parallel to the isobars
  • the air flow aloft is neither into L nor away
    from H.
  • Air flow at the surface is across the isobars.
  • air convergence near low pressure centers
  • air divergence near high pressure centers

Where does it go?
Where does it come from?
7
Vertical structure of deep dynamic lows
  • The air cannot disappear or come out of nowhere
    the surface flow is related to the vertical flow
    and consequently to the air flow aloft.
  • The surface winds are coupled to the winds aloft
  • What type of upper-level air flow would favor the
    formation and development of a surface wave
    cyclone?

8
Favorable conditions for a strong midlatitude
storm
  • Air convergence at the
  • surface is aligned with air
  • divergence aloft.
  • Air divergence at the
  • surface is aligned with
  • area of convergence aloft
  • Surface L intensifies (weakens) if the
    divergence aloft is stronger (weaker) than the
    surface convergence.
  • Surface H intensifies (weakens) if the
    convergence aloft is stronger (weaker) than the
    surface divergence.

9
But
  • We know that at upper levels the winds are
    blowing along the isobars.
  • The air aloft is NOT converging into nor it is
    diverging away from pressure centers (L or H).
  • What is the right pattern of the upper level
    winds that will result into a strong storm?

10
Is it this one?
  • Low over Low,
  • High over High.
  • No convergence or
  • divergence aloft.
  • The surface Low will
  • fill up and disappear
  • The surface High will be
  • depleted and disappear
  • Such a configuration
  • does NOT support the storm.
  • Similarly, Low over High, High over Low wont
    work.
  • Surface and upper-level pressure centers cannot
    be aligned above each other.

11
Is it this one?
  • Perfect geostrophic flow parallel isobars,
    constant wind speed
  • Again, no divergence or convergence (i.e. piling
    up or removal of air).
  • This configuration will NOT support a strong
    storm at the surface
  • Conclusion the isobars must curve, creating
    regions where they spread apart and/or get closer
    together.

12
500 mbar pressure map
  • The air converges as it flows toward the L
    trough.
  • The air diverges as it flows away from the L
    trough.

Convergence
Divergence
13
Upper Level Waves
  • Long waves (Planetary, Rossby waves)
  • Typically the longwaves have 3-6 wavelengths
    around the Earth.
  • The result from the uneven heating of the Earth
    and the rotation of the planet.
  • Long waves move very slowly or are stationary.
  • Often created by mountain ranges
  • Shorter waves
  • Imbedded in the long waves
  • Short waves travel faster
  • They can intensify the troughs of the long waves.

14
The Vertical Structure of a Middle-latitude Storm
  • The surface L is aligned with the diverging part
    of the jet stream flow.
  • The surface H is aligned with the converging part
    of the jet stream flow.
  • H and L centers are not aligned! Upper-level
    centers are generally shifted to the west

15
Another way of looking at it.
16
Another way of looking at it
  • B) storm intensifies convergence over surface H,
    divergence over surface L.
  • C) storm dies out Low over Low.

17
Summary of the Processes in a Cyclonic Wave
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