tornadogenesis: unknowns erik rasmussen, rasmussen systems jerry straka, ou kathy kanak, cimms 2009...

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Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

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Page 1: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Tornadogenesis:Unknowns

• Erik Rasmussen, Rasmussen Systems• Jerry Straka, OU• Kathy Kanak, CIMMS

2009 College of DuPage Storm Conference

Page 2: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. A violently rotating column of air, in contact with the ground, either pendant from a cumuliform cloud or underneath a cumuliform cloud, and often (but not always) visible as a funnel cloud.

Page 3: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Tornadoes and Tornado Cyclones

• What are they and why should we care?

Page 4: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. A violently rotating column of air, in contact with the ground, either pendant from a cumuliform cloud or underneath a cumuliform cloud, and often (but not always) visible as a funnel cloud.

What is violent?Vortices generally increase in windspeed as they contract in radius. So intensity is partially dependent on the degree of contraction.

Page 5: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. A violently rotating column of air, in contact with the ground, either pendant from a cumuliform cloud or underneath a cumuliform cloud, and often (but not always) visible as a funnel cloud.

Funnel vs. tornado issue?Note Markowski et al. (MWR 2002, pp. 1692-)

Page 6: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. A violently rotating column of air, in contact with the ground, either pendant from a cumuliform cloud or underneath a cumuliform cloud, and often (but not always) visible as a funnel cloud.

Probably to filter against dust devils, etc.“Pendant” is essentially impossible from a physical perspective.

Page 7: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. A violently rotating column of air, in contact with the ground, either pendant from a cumuliform cloud or underneath a cumuliform cloud, and often (but not always) visible as a funnel cloud.

A funnel cloud is a condensation pressure surface within a vortex. It is not the vortex itself, which physically must be larger than the funnel.

Page 8: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

tornado—1. I know one when I see one.

Page 9: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

A B

B

A

Page 10: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Angular momentum M=Vr = tangential, swirling velocity times radius. Dimmitt tornado, 2 June 1995. From single-Doppler analysis. M=14000 contour

Page 11: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Approximate swirling windspeed and angular momentum in the Dimmitt tornado early in mature stage about 200 m above the ground.

Page 12: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference
Page 13: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

This flow would evolve from the previous in < 5 minutes with a modest inflow of (e.g.) about 5 m/s at 500 m radius

Page 14: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

As the high-M air penetrates closer to the axis, maximum swirling wind speed ~doubles for each halving of the radius of penetration of the large M region.

Page 15: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Thoughts...• Most supercells probably have

tornado cyclones. Nomenclature isn't so important as understanding that...

• A tornado, whatever wind speed or appearance criteria that are used, is the inner portion of a tornado cyclone where enough angular momentum has been transported toward the axis to give tornadic windspeeds.

Page 16: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Thoughts...• Tornadogenesis failure is possibly

simply a failure of contraction of the tornado cyclone.

• Strength of the inner portion of the vortex (the tornado) depends on angular momentum in the outer portion, and the removal of mass upward through the vortex (and hence convergence below).

Page 17: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Thoughts...• Hence we seek to understand why most

supercells are not conducive to transporting sufficient air upward through the tornado cyclone to increase the vortex to tornado strength.

• Operationally, if tornado cyclones are even close enough to the 88D for detection, the differences between tornadic and non-tornadic TCs may almost always lie at unresolvable scales.

Page 18: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Thoughts about EF scale and tornado windspeeds (needed?)

• See if this can be tied to the science of the talk; else delete.

Page 19: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

So how did the Tornado Cyclone come into existence?

• Here are some historically validated observations about the supercell:

Page 20: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Common supercell features:

• Updraft acquires horseshoe shape.• Counter-rotation is observed.• A Rear-Flank Downdraft is present in

the interior of the horseshoe pattern.• The tornado cyclone is centered in

strong vertical velocity gradient on the interior left edge of the horseshoe.

• A gust front is present below the rear edge of the updraft.

Page 21: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference
Page 22: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference
Page 23: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference
Page 24: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

A simulation...

Horseshoe-shaped updraft

Rear-Flank Downdraft

Counter-rotating vortices

Vortex straddles up/downdraft

Page 25: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Initial conditions

Page 26: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

RFDs

• Again, classification may get in the way. Occlusion downdraft vs RFD; buoyancy vs. dynamic.

• Back to Markowski... DD must be involved.

• Q2: RDF forcing• Q1: RFD buoyancy vs. height• Q3: Rear-side precipitation role

Page 27: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

RFDs

• Arching vs tilting of near-ground inflow... is either necessary? Is either sufficient?

Page 28: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Tornado longevity

• Is the tornado just a spin-down process of TC.

• Is a tornado maintained somehow (and maybe is a TC maintained somehow)?

• Degree of occlusion?• WHy shorter-track before longer-

track?• (Track length product of duration and

forward motion; is duration the key scientific issue?

Page 29: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Role of the Mesocyclone

• Not direct?• Straka et al. Already showed that very

“tornadic looking” features can be formed when precip occurs at the side of an updraft IN TOTAL ABSENCE OF FLOW HENCE SHEAR

• Is the role of a meso to deposit precip at a location that is effective for arching?

Page 30: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

The supercell environment

• Deep environmental structure• Near-ground importance• Why flee big CAPE (you don't need no

Shtinkin' CAPE)• Why does big CAPE seem to be

special on some days?• Alternative hypotheses, and the

earlier studies• [Check blog post to students]

Page 31: Tornadogenesis: Unknowns Erik Rasmussen, Rasmussen Systems Jerry Straka, OU Kathy Kanak, CIMMS 2009 College of DuPage Storm Conference

Thank you!

This research is supported by you through the National Science Foundation

[email protected]://www.rasmsys.com