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Davies-Jones, 1984

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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. - PowerPoint PPT Presentation
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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
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Page 1: Davies-Jones, 1984

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 2: Davies-Jones, 1984

Storm-relative Environmental Helicity (SREH)

(actually, streamwise vorticity)

Page 3: Davies-Jones, 1984

Unidirectional shear (straight hodograph): mean motion on hodograph implies no SREH…..need to develop off-hodograph propagation to develop storm updraft rotation

Directionally varying shear vector(curved hodograph): mean motion off hodograph implies rotating storm updraft from get-go

Page 4: Davies-Jones, 1984

Vertical wind shear: updraft rotation develops as result of tilting and subsequent stretching of environmental horizontal vorticity, producing dynamic PGFs that promotes the maintenance and propagation of the rotating storm (Gallilean invariant)

SREH: assumes steady, propagating updraft and deduces updraft rotational characeristics based on storm motion (not Gallilean invariant)

Supercell Perspectives:

Page 5: Davies-Jones, 1984

Thompson et al., WAF 2012

EBWD

EBWD: Effective Bulk Wind Difference (half storm depth)

Convective Modes

Page 6: Davies-Jones, 1984

Thompson et al., WAF 2012

Convective Modes

ESRH

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

Page 7: Davies-Jones, 1984

Potential Vorticity:

= 0 for isentropic motions

Equivalent Potential Vorticity:

Page 8: Davies-Jones, 1984

For a horizontally homogeneous atmosphere with vertical wind shear, vortex lines and Theta-E surfaces are initially horizontal (EPV=0). Since EPV is conserved, vortex lines remain on the original theta-E surfaces if they are subsequently tilted up or down…. Thus, vertical vorticity generated via tilting must be colocated within a horizontal gradient of theat-E!

Equivalent Potential Vorticity:

Page 9: Davies-Jones, 1984

Supercells

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“On the rotation and propagation of simulated supercell thunderstorms” Rotunno and Klemp, JAS, 1985

…… used unidirectional shear

Page 13: Davies-Jones, 1984

Z = 4 km

Z = .25 km

W, Qr

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Vorticity Equation:

Vertical Vorticity:

tilting stretching

2D Horizontal Vorticity:

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Vortex Tube

Circulation:

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Rotunno and Klemp, JAS, 1985

Unidirectonal shear, Warm rain

…surface mesocyclone formed from tilting of horizontal vorticity generated in storm’s forward flank region

Page 23: Davies-Jones, 1984

Supercells

Page 24: Davies-Jones, 1984

Klemp and Rotunno, JAS, 1983

1 way nest, adjustment from 1km to 250m, 6 min simulation….

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Adlerman and Droegemeier JAS 1999

100 km x 100 km, 500 m grid

Back to Del City…. 20 May, 1977

“Cyclic- Mesocyclogenesis”

Page 29: Davies-Jones, 1984

Adlerman and Droegemeier, MWR, 2005

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