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Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

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Page 1: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Solid body rotation (XY):

Divergent flow (XY):

Shear flow (XY):

low pressure

high pressure

*no pressure perturbation

Page 2: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Splat:

Spin:

(stagnation pressures near saddle pts. in streamline pattern)

(eddy rotation)

For flow in solid body rotation:

Page 3: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

2D Supercells??

2D Vorticity Eq.

2D Diagnostic Pressure:

No tilting, stretching!!

No rotationally-induced mid-level mesolow

Page 4: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

A Simple “Model” of a Tornado:

Rankine Combined Vortex:

Cyclostrophic balance:

Solid-body rotation in core:

Potential vortex outside:

*For core region:

For full vortex:

Page 5: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Vmax=10 ms-1

Vmax=20 ms-1

Vmax=40 ms-1

.5 hPa

2 hPa

8 hPa

.5 K

2 K

8 K

For Vortex at 3 km AGL:*

*simply assuming pressure change from inner-core region

Page 6: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

at rmax:

beyond rmax:

…for Rankine vortex:

Vrmax=40 ms-1 V20= 20 ms-1

Page 7: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Ordinary Cell:

Page 8: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Multicell:

Page 9: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Supercell:

Page 10: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 11: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

•Buoyancy processes: basic updraft/downdraft, (ordinary cells)

•Gust front processes: triggering of new cells, upscale growth, (multicells)

•Dynamic processes: rotating updraft, dynamic vertical pressure gradient forcing, (supercells)

Physical processes controlling cell types:

Page 12: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Basic Equations:

(Buoyancy)--

+ ice….

Page 13: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Buoyant Processes:

Page 14: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Buoyancy is Scale-Dependent!!!

…real bubble in 3D simulation

Page 15: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 16: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Theoretical speed of propagation:

Density Currents

Page 17: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

“Optimal” condition for cold pool lifting

C/∆u > 1

C/∆u = 1

C/∆u < 1

RKW Theory

Rotunno et al. (JAS, 1988)

Page 18: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 19: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Dynamic Pressure Effects:

Dynamic pressure Buoyancy pressure

Vertical momentum:

(take divergence)

diagnostic pressure eq.

Page 20: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

~

Updraft growing in sheared environment:

Page 21: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Vorticity Equation:

Vertical Vorticity:

tilting stretching

Page 22: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Vortex Tube

Circulation:

Page 23: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 24: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 25: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 26: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

~

Page 27: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 28: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 29: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Supercell processes are Galilean invariant!!!

Supercell Hodographs:

Page 30: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Bunkers et al. WAF 2000

Page 31: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Potential Vorticity:

= 0 for isentropic motions

Equivalent Potential Vorticity:

Page 32: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Davies-Jones, 1984…from linear theory of circular, convective cells in a sheared environment, covariance of vertical velocity and vertical vorticity is proportional to the storm-relative environmental helicity

*assumes steady-state, propagating storm

Page 33: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Storm-relative Environmental Helicity (SREH)

(actually, streamwise vorticity)

Page 34: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Thompson et al., WAF 2012

EBWD

EBWD: Effective Bulk Wind Difference (half storm depth)

Convective Modes

Page 35: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Thompson et al., WAF 2012

Convective Modes

ESRH

ESRH: Effective Storm-Relative Helicity (effective inflow layer)

Page 36: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 37: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Vortex Tube

Circulation:

Page 38: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 39: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 40: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 41: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 42: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Adlerman and Droegemeier, MWR, 2005

Page 43: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 44: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 45: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 46: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Ward Tornado Chamber (1972)

Ingredients for a tornado: 1) source of rotation

2) updraft

Page 47: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 48: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 49: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Swirl Ratio: S = Vo / Wo

Page 50: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 51: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 52: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation
Page 53: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

McCaul MWR 1991

Page 54: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

McCaul and Weisman MWR 1996

Page 55: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

McCaul and Weisman MWR 1996

Page 56: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation

Thompson et al., WAF 2012

STP

STP: Sig. Tornado Parameter

Page 57: Solid body rotation (XY): Divergent flow (XY): Shear flow (XY): low pressure high pressure *no pressure perturbation