Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES...

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Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA RESEARCH CENTER FOR ENVIRONMENTAL CHANGES ACADEMIA SINICA TAIPEI, TAIWAN 2014-04-08 EUMETSAT CWG WORKSHOP, ZAGREB, CROATIA

Transcript of Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES...

Page 1: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Dynamical processes at the storm top

PAO K. WANGDEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES

UNIVERSITY OF WISCONSIN-MADISONMADISON, WISCONSIN, USA

RESEARCH CENTER FOR ENVIRONMENTAL CHANGESACADEMIA SINICA

TAIPEI, TAIWAN

2014-04-08 EUMETSAT CWG WORKSHOP, ZAGREB, CROATIA

Page 2: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

collaborators

Kai-Yuan Cheng

Tempei Hashino

Martin Setvak

Maria Putsay

Zdenek Charvat

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Satellite observed features of storm tops

• The features shown at the top of a storm is the combined result of many different physical processes

• If we can explain the formation of these features, we can understand better the development of thunderstorms

• We can also use such knowledge to nowcast the storm behavior

Page 4: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Some storm top features recently examined

• Above anvil cirrus plumes

• Cold-U(V)

• Cold area (CA)

• Closed-in warm area (CWA)

• Warm-cold couplet

• Cold rings

• Warm trenches

• Ship waves

Page 5: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Basic dynamic processes of deep convection

• Air parcel rapidly rises from the boundary layer to the tropopause level, and often overshoot, to release the instability

• Part of the KE carried by the parcel is used to excite internal gravity waves (IGW) near the storm top when the parcel encounters the stable stratosphere

• The interaction among updraft, ambient wind, and IGW is largely responsible for most storm top features as observed by meteorological satellites.

Page 6: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.
Page 7: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.
Page 8: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Cold-V, CWA, warm-cold couplet, distant warm area

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Interaction between ambient wind and updraft

Page 10: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.
Page 11: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.
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Weak wind shear – cold ring

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Something is going on…warmer doesn't necessarily mean lower

1500 sec

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If we set U = 0a symmetric cold ring appears

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HIGHER BUT WARMER ?!Wave breaking and mixing

1800 sec

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Masking effect of plumes

Page 17: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Above anvil cirrus plumes

plume

Anvil

Storms over Balearic Islands

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Above anvil cirrus plumesInstability and Wave Breaking

Convection-induced instability and gravity wave breaking at the storm top send H2O through the tropopause to enter the stratosphere.

Overshooting top plumes Anvil wave breaking

Wang (2007)

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Wang et al. (2011)

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Courtesy of Zdenek Charvat

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Ship wavesobstacle effect of storms

Page 23: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Latest example of storm top ship waves from Suomi NPP image

Courtesy of Kris Bedka

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Radial cirrus features

Setvak et al., 2013

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Putsay et al., 2009

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Courtesy of Maria Putsay

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Courtesy of Maria Putsay

Page 32: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Wave in a moving fluidwind

Page 33: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.

Courtesy of Martin Setvak

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Interference of wavessame phase, frequency, amplitude, no wind

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Same phase, frequency, amplitude, constant wind

2 point sources. D = 3.5 lambda

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u

D = 1.5 lambda

D = 2 lambda

D = 3.5 lambda

D = 4 lambda

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3 sources (i.e., 3 Ots)

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Page 39: Dynamical processes at the storm top PAO K. WANG DEPARTMENT OF ATMOSPHERIC AND OCEANIC SCIENCES UNIVERSITY OF WISCONSIN-MADISON MADISON, WISCONSIN, USA.
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Implications

Cbs with radial cirrus features possibly have two or more overshooting tops

The IGW caused by different OTs interfere which causes the quasi-radial pattern

Interference enhances wave amplitude, hence stronger CAT above the storm may be expected

Above storm layer is possibly more humid than previously thought

Do the presence of multiple OTs indicate a more intense storm?