1. Middle Latitude Cyclones This chapter discusses: 1.The location, vertical structure, and developmental stages of middle latitude cyclones 2.How upper level convergent winds, abrupt topographic features, and planetary longwaves may enhance cyclonic development at the surface

2. Polar Front Theory – Wave Cyclone Cycle Stage 1 Frontal Wave Overrunning Precipitation Open Wave Stage 3 Stage 2 Stage 1: One explanation for development of middle latitude cyclones begins with a stationary front with warm and cold winds in opposite directions (e.g. wind shear). Stage 2: A wavelike kink, such as a low pressure system creates a frontal wave, or incipient cyclone under the right conditions. Stage 3: As the storm develops into an open wave, a broad band of precipitation forms ahead of the warm sector.

3. Energy driving their development originates from kinetic sources such as rising warm air, sinking cold air, and converging air, as well as latent heat of condensation. Stage 4: When occlusion occurs when cold air lies on both sides of the occluded front. Without an ample supply of energy of rising, warm, moist air, the system will dissipate. Stage 5: The end stage is where precipitation-free area is observed. In addition, only a weak cyclonic circulation is seen in the wind field. Stage 4 Stage 3a Stage 5

4. Wave Cyclone Development A series, or family, of cyclones, at various stages of development, may extend across North America.A series, or family, of cyclones, at various stages of development, may extend across North America. Energy driving their development originates from kinetic sources such as rising warm air, sinking cold air, and converging air, as well as latent heat of condensation.Energy driving their development originates from kinetic sources such as rising warm air, sinking cold air, and converging air, as well as latent heat of condensation. Baroclinic instability drives the middle latitude cyclones even further.Baroclinic instability drives the middle latitude cyclones even further.

5. Baroclinic instability arises from temperature advection. Where on the globe is there an overall strong thermal gradient and why?

6. Cyclone & Anticyclone Paths Many well known paths for low and high pressure systems extend across North America, and their interaction helps develop the open wave cyclone.Many well known paths for low and high pressure systems extend across North America, and their interaction helps develop the open wave cyclone. Cyclogenesis describes the strengthening or development of these storms into huge unstable waves.Cyclogenesis describes the strengthening or development of these storms into huge unstable waves. Cyclones developing on the eastern slopes of the Rockies are called lee- side lows and are sometimes associated with redevelopment of previous systems come onshore from the Pacific Ocean.Cyclones developing on the eastern slopes of the Rockies are called lee- side lows and are sometimes associated with redevelopment of previous systems come onshore from the Pacific Ocean.

7. 4 main stages in Cyclogenesis

8. Initial Development of Wave Cyclone Jet streak upstream of short-wave trough (often diffluent) Sinking motion upstream of trough axis PVA aloft over incipient surface low Weak surface system downstream of short-wave trough Elongated area of clouds (baroclinic leaf) parallel to mid-level flow Near surface low center: low-level convergence, upper-level divergence, rising motion, and pressure falls

9. Rapid Development Stage 500 hPa trough amplifies (height falls west of trough axis and height rises downstream ) Cyclonic circulation results in warm advection to east and cold advection to west of surface low Temperature advection yields dipole vertical motion field Comma cloud develops Surface pressures fall due to net warming of column (low-level WAA + tropopause undulation) Surface low moves east- northeast towards greatest pressure falls and max upward motion

10. Mature (Open Wave) Stage mid-tropospheric flow changes dramatically; trough becomes negatively tilted SW flow increases SW of surface low Absolute vorticity increases Jet core migrates to southwest of surface Expansion of clouds around warm front and west of surface low Narrower cloud band along and behind cold front Some western clouds are Sc by mixing Dry slot develops due to subsidence; part of dry conveyor belt and high IPV air entering system

11. Occluded (Maximum Intensity) Stage Center cut off from warm sector Cold air at mid-lower levels over cyclone 500 hPa vorticity maximum near surface low center “Stacked” system in vertical – advections are small Broad west-east cloud shield Occlusion not completely due to cold front catching up to warm front – but to low moving into cold air due to dynamic processes Increasing ascent NW of low + cold advection yields thickness minimum which coincides with cyclone center Warm air in upper trop/lower stratosphere overlays cold mid-lower tropospheric air, allows pressures to fall

12. Lee-Side Cyclone As westerly winds flow over a mountain range, the airflow is deflected to the south initially. These air parcels after traversing over the mountain range will reemerge with a northeasterly path. This motion leads to a formation of a semi-persistent trough feature on the eastern plains of Colorado called a lee- side trough. If there is enough upper-level support, this setup can develop even further and creating a lee-side low. This concept is associated with the “conservation of potential vorticity.”

13. Convergence & Divergence Rapid intensification of cyclones is prohibited when low pressure aloft is directly above the surface low.Rapid intensification of cyclones is prohibited when low pressure aloft is directly above the surface low. In this scenario, the convergence at the surface low builds up air pressure and fills in the low with excessive mass.In this scenario, the convergence at the surface low builds up air pressure and fills in the low with excessive mass. The same stacking of high pressure, with divergence at the surface, will weaken the anticyclone.The same stacking of high pressure, with divergence at the surface, will weaken the anticyclone. In order for a surface cyclone to strengthen, a high pressure must be over it and vice versa for a surface high pressure.In order for a surface cyclone to strengthen, a high pressure must be over it and vice versa for a surface high pressure. This configuration will allow for mass to be transported through the atmosphere and promote a constant up or downward vertical motion.This configuration will allow for mass to be transported through the atmosphere and promote a constant up or downward vertical motion. Idealized case for cyclogenesis Not idealized case for cyclogenesis

14. Storm Vertical Structure Divergence of air aloft occurs as height contours intervals widen.Divergence of air aloft occurs as height contours intervals widen. Low pressure systems deepen and intensify (e.g. cyclogenesis) when upper-level divergence is stronger than the surface convergence, which requires a vertical staggering of surface and upper lows.Low pressure systems deepen and intensify (e.g. cyclogenesis) when upper-level divergence is stronger than the surface convergence, which requires a vertical staggering of surface and upper lows. When more air converges at the surface than it is removed at the top, this signifies a storm is filling or dissipating and weakening as surface pressure rises.When more air converges at the surface than it is removed at the top, this signifies a storm is filling or dissipating and weakening as surface pressure rises.

15. Divergence and Convergence Convergence or confluence of air aloft creates downward motion. Divergence or diffluence of air aloft generates upward motion. DIV = Divergence CON = Convergence

16. Upper Level Waves Earth's poles are encircled by 3 to 7 longwaves, or Rossby waves, directing upper level winds around lows at the 500 mb surface.Earth's poles are encircled by 3 to 7 longwaves, or Rossby waves, directing upper level winds around lows at the 500 mb surface. Longwaves or Rossby waves are more trend maker than weather maker.Longwaves or Rossby waves are more trend maker than weather maker. Small disturbances in these Rossby waves can trigger storms.Small disturbances in these Rossby waves can trigger storms.

17. Shortwave Disturbance Shortwave troughs within the larger Rossby wave move faster, and propagate downwind into the Rossby troughs and cause them to deepen.Shortwave troughs within the larger Rossby wave move faster, and propagate downwind into the Rossby troughs and cause them to deepen. Barotropic conditions, where height contours and isotherms are parallel (no temperature advection) dominate in Rossby waves.Barotropic conditions, where height contours and isotherms are parallel (no temperature advection) dominate in Rossby waves. Within shortwaves, the height contours and isotherms are usually slight out of phase creating temperature advection.Within shortwaves, the height contours and isotherms are usually slight out of phase creating temperature advection. A shortwave can deepen or amplify a longwave collapse into a baroclinic state.A shortwave can deepen or amplify a longwave collapse into a baroclinic state.

18. General Characteristics: Long Waves Short Waves Number of Waves 3-7 across hemisphere; typically 4-5 ~ 15º-40º long. wide, move through long wave troughs Amplitude Meridionally, on the order of several 1000 km Meridionally, on the order of several hundred km, up to 1000 km Wavelength ~50-120  longitude~10-40  longitude Diagnosed best at At 500 hPa and aboveAt 500 hPa and below Movement Generally eastward at 10-15 knots; but can remain quasi- stationary or even retrogress Dominantly eastward with a northerly or southerly component; faster than the long wave troughs Energy Regime Barotropic or Equivalent Barotropic Definitely baroclinic

19. 1530 m 1500 m 10  C 5C5C VgVg Weak Baroclinicity - Weak Temperature Advection

20. VgVg Strong Baroclinicity - Strong Temperature Advection 1530 m 1500 m 0C0C 5C5C

21. VgVg No Baroclinicity - No Temperature Advection (Equivalent Barotropic Atmosphere) 1530 m 1500 m 10  C 5C5C

22. L L L L Vertical Baroclinicity – Tilting of the System with Increasing Heights Cold z x

23. Classic ETC Model – Open Wave L sfc L 500 Warm Sector

24. Classic ETC Model – Occlusion L sfc L 500 Warm Sector

25. Cyclone Development: Upper Winds A) B) C)

26. Atmospheric conditions at the surface and aloft affect cyclogenesis.Atmospheric conditions at the surface and aloft affect cyclogenesis. An upper level shortwave can trigger baroclinic instability, which converges flow aloft upstream, raises high pressure, and supports cold air advection.An upper level shortwave can trigger baroclinic instability, which converges flow aloft upstream, raises high pressure, and supports cold air advection. Downwind, divergent flow aloft deepens the surface low, and warm advection increases rising air flow.Downwind, divergent flow aloft deepens the surface low, and warm advection increases rising air flow. Eventually the system occludes.Eventually the system occludes.

27. Jet Streak Influence Divergence aloft is enhanced by the polar front and/or subtropical jet streams, where the jet maximum, or jet streak, forms in the tightly packed gradients.

28. Jet Streak Convergence & Divergence Jet streaks can help to intensify a surface cyclone even farther.Jet streaks can help to intensify a surface cyclone even farther. The polar front or subtropical jet streak forces air convergence aloft upstream of the deepening open wave cyclone, and then divergence downstream where the surface cyclone is located.The polar front or subtropical jet streak forces air convergence aloft upstream of the deepening open wave cyclone, and then divergence downstream where the surface cyclone is located. When these wind maximums are gone, the cyclone degrades.When these wind maximums are gone, the cyclone degrades.

29. 90 kt 70 kt Movement of the Jet Streak Right Front Region Upward Motion Right Exit Quadrant Downward Motion Left Exit Quadrant Upward Motion Left Front Region Downward Motion

30. Summary of Cyclone Weather Upper and surface maps illustrate the role of convergence and divergence aloft, and the pattern of clouds, precipitation, and temperatures on the ground. A mid-latitude cyclone experiences its maximum intensity when the upper-level low or trough is juxtaposed to the northwest of the surface low pressure. The upper- and lower-level lows are tilted vertically to provide for the maximum upward vertical motion.

31. Conveyor Belt Model This model describes rising and sinking air along three conveyor belts, warm conveyor belt rises with water vapor above the cold conveyor belt which also rises and turns.This model describes rising and sinking air along three conveyor belts, warm conveyor belt rises with water vapor above the cold conveyor belt which also rises and turns. Finally the dry conveyor belt descends brining clearer weather behind the storm.Finally the dry conveyor belt descends brining clearer weather behind the storm. Old Model Old but Slightly Revised Model

32. Ng (2005) Doctoral Dissertation Revised View of Conveyor Belts Illustrating 3-D Deformation

33. Comma Clouds Rising and turning moist air, illustrated in the conveyor belt model, condenses into a large comma-shaped cloud typical of the open wave cyclone.Rising and turning moist air, illustrated in the conveyor belt model, condenses into a large comma-shaped cloud typical of the open wave cyclone. This March 1993 storm wreaked havoc along the East Coast.This March 1993 storm wreaked havoc along the East Coast.

34. 3/93 Storm Size & Pressure For the storm of the century, the low pressure center reached 980 mb, and the storm extended across several southeastern states.

35. 3/93 Storm Temperature Advection Upper level winds flowed along a deep trough with steep baroclinic cold and warm air advection.

36. Storm of Century Path Low pressure values and location are charted with time to illustrate the storm track and intensity, moving from Texas to Maine in 2 days.

37. Vorticity & Cyclone Spin Vorticity describes the spin of an air parcel, which is positive in counterclockwise cyclonic flow.Vorticity describes the spin of an air parcel, which is positive in counterclockwise cyclonic flow. Due to the conservation of angular momentum, vorticity increases with a decrease in parcel radius (e.g. stretching due to divergence aloft) (local vorticity) and increase in earth's latitude (earth’s vorticity).Due to the conservation of angular momentum, vorticity increases with a decrease in parcel radius (e.g. stretching due to divergence aloft) (local vorticity) and increase in earth's latitude (earth’s vorticity).

38. 4 Types of Vorticity Relative (local)Relative (local) Earth’s (Coriolis parameter; f =2  sin  )Earth’s (Coriolis parameter; f =2  sin  ) Absolute (local + earth’s)Absolute (local + earth’s) Potential (absolute + depth)Potential (absolute + depth)

39. Sources of Vorticity Curvature of upper level heights and winds, as well as strong changes in wind speed, or shear, generate the spin of relative vorticity.Curvature of upper level heights and winds, as well as strong changes in wind speed, or shear, generate the spin of relative vorticity. Additional earth’s vorticity is generated by the earth's spin, and together they comprise absolute vorticity.Additional earth’s vorticity is generated by the earth's spin, and together they comprise absolute vorticity.

40. y x      Curvature Vorticity

41. y x Shear Vorticity

42. y x as vorticity decreases, area increases Absolute Circulation = Constant = Absolute Vorticity x Area as vorticity increases, area decreases DIV CON

43. Trough to Ridge Vorticity Change Anticyclonic spin around a ridge reduces absolute vorticity, but the convergence and cyclonic spin in the trough enhance the relative vorticity and hence increases absolute vorticity as well

44.  +    + 2    Con+ Con Div+ Div

45. PVA NVA NVAPVA Maximum  at the base of the trough: Maximum  at the base of the trough:  > 0;  > 0 Minimum  at the crest of the ridge: Minimum  at the crest of the ridge:  > 0 30  N 35  N 40  N 45  N

46. Vorticity & Vertical Motion The 500 mb map vorticity maximum is a signal that to its east, air is diverging aloft.The 500 mb map vorticity maximum is a signal that to its east, air is diverging aloft. If there is also convergence below, then an open wave cyclone will likely deepen. If there is also convergence below, then an open wave cyclone will likely deepen. Hence, 500 mb charts are useful in analyzing “vorticity maximum” and predict potential storms in a quick, crude way. Hence, 500 mb charts are useful in analyzing “vorticity maximum” and predict potential storms in a quick, crude way.

47. Vertical Storm Profile Surface, 500 mb, and 200 mb charts are used to illustrate the structure of the February 1983 open wave cyclone exploding over North Carolina. The 500 mb chart shows a shortwave dashed line moving into the longwave trough and baroclinic cold air advection.

48. February 1983 Vorticity Lines of equal vorticity are plotted on the 500 mb chart for the February 1983 open wave cyclone that buried the east coast in snowfall.Lines of equal vorticity are plotted on the 500 mb chart for the February 1983 open wave cyclone that buried the east coast in snowfall. Note that the “vort max” is west of the storm center, strengthening the cyclogenesis.Note that the “vort max” is west of the storm center, strengthening the cyclogenesis.

49. Imaging Vorticity Centers GOES West satellite infrared imagery of water vapor are useful in identifying swilling vorticities, seen off Pacific Northwest coast.

50. Potential Vorticity = Absolute Vorticity / Depth = Constant PV  0: D   < 0 PV > 0: D   > 0 TROPOPAUSE

51. Maximum  at the windward side of the mountain:  > 0;  > 0 Minimum  at the top of the mountain: Minimum  at the top of the mountain:  < 0;   0 Maximum  at the leeward side of the mountain:  > 0;  > 0 acquiring anticyclonic curvature acquiring cyclonic curvature

52. Polar Lows Cyclones that develop above the polar front, called polar lows, are smaller in size than mid-latitude cyclones.Cyclones that develop above the polar front, called polar lows, are smaller in size than mid-latitude cyclones. They form during the winter, have warm central cores, strong winds, and generate snow.They form during the winter, have warm central cores, strong winds, and generate snow. Size ~ 1000 to 500 kmSize ~ 1000 to 500 km Eye-like clear structure similar to a hurricane with the most intense winds and precipitation near the eye core.Eye-like clear structure similar to a hurricane with the most intense winds and precipitation near the eye core.