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Boundary-layer turbulence, surface processes, and orographic precipitation growth in cold clouds or: The importance of the lower boundary Qun Miao Ningbo University Bart Geerts University of Wyoming CAR orographic precip workshop, 13-15 March 2012 cknowledgements: Yang Yang, UWKA crew, Roy Rasmussen, Dan Breed

Qun Miao Ningbo University Bart Geerts University of Wyoming

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Boundary-layer turbulence, surface processes, and orographic precipitation growth in cold clouds o r: T he importance of the lower boundary. Qun Miao Ningbo University Bart Geerts University of Wyoming. acknowledgements: Yang Yang , UWKA crew, Roy Rasmussen, Dan Breed. - PowerPoint PPT Presentation

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Page 1: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Boundary-layer turbulence, surface processes, and orographic precipitation growth in cold clouds

or:The importance of the lower boundary

Qun MiaoNingbo University

Bart GeertsUniversity of Wyoming

NCAR orographic precip workshop, 13-15 March 2012

acknowledgements: Yang Yang, UWKA crew, Roy Rasmussen, Dan Breed

Page 2: Qun Miao Ningbo University Bart  Geerts University of Wyoming

The advantage of a nadir view …

radar+lidarradar+lidar

radar only

vertical plane dual-Doppler below flight level

• Wyoming Cloud Radar• Wyoming Cloud Lidar

Page 3: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Does boundary-layer turbulence enhance snow growth in mixed-phase

clouds?

Med Bow Mtns

Med Bow Mtns

wind

Page 4: Qun Miao Ningbo University Bart  Geerts University of Wyoming
Page 5: Qun Miao Ningbo University Bart  Geerts University of Wyoming

(equivalent) potential temperature (K)

mean echo top height (km MSL) 6.2mean wind speed (m s-1) 20mean Brunt-Väisälä frequency (10-2 s-1) 1.02

mean shear (10-3 s-1) 9.2mean Froude number 1.4mean Richardson number 1.3mixing ratio at 200 m AGL (g kg-1) 3.1mean LCL (km MSL) 2.78mean LCL temperature (°C) -5

𝑅𝑖= 𝑁 2

( 𝜕𝑈𝜕 𝑧 )2

300 mb height, 800 mb T & wind barbs

Page 6: Qun Miao Ningbo University Bart  Geerts University of Wyoming

turbulent BL depth: ~ 1.0 km

power spectrum over this WCR section

Page 7: Qun Miao Ningbo University Bart  Geerts University of Wyoming

(equivalent) potential temperature (K)

mean echo top height (km MSL) 4.4mean wind speed (m s-1) 12mean Brunt-Väisälä frequency (10-2 s-1) 0.2

mean shear (10-3 s-1) 3.8mean Froude number 5mean Richardson number 0.4mixing ratio at 200 m AGL (g kg-1) 2.6mean LCL (km MSL) 2.6mean LCL temperature (°C) -8

Page 8: Qun Miao Ningbo University Bart  Geerts University of Wyoming

turbulence top = cloud top

Page 9: Qun Miao Ningbo University Bart  Geerts University of Wyoming

distance (km)

Does this turbulence really matter

brief spells of snow growth by accretion or riming in rising eddies?

Page 10: Qun Miao Ningbo University Bart  Geerts University of Wyoming

time (UTC)

2009-03-10

B

B

Page 11: Qun Miao Ningbo University Bart  Geerts University of Wyoming

surface-induced snow initiation ??

Page 12: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Composite analysis of snow growth, based on 10 flights over the Med Bow Range in SE Wyoming,using CFADs

black lines: along-wind legs

red lines: ladder pattern

Page 13: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Frequency by altitude (FAD) plotsal

titud

e ab

ove

the

grou

nd

reflectivity or vertical velocitybin Dz

bin

Z or

V in

crem

ent

nn

(Yuter & Houze 1997)

date 18 Jan 06

27-28 Jan 06

2 Feb 06

11 Feb 08

25 Feb 08

18 Feb 09

20 Feb 09

10 Mar 09

25 Mar 09

30 Mar 09

# along-wind flight legs 5 17 10 2 3 3 2 4 4 3

# ladder legs 0 0 0 16 16 16 12 14 14 12

Page 14: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Med Bow Range

crest

LCL

wind

1.upwind

below LCL

2.upwind

above LCL3.lee

4.4 5.9 5.9 107 profileswest east

Page 15: Qun Miao Ningbo University Bart  Geerts University of Wyoming

WCR reflectivity (dBZ)

crest

LCL

Page 16: Qun Miao Ningbo University Bart  Geerts University of Wyoming

1 23

123

1 2 3

crest

LCL1 2 3

1. rapid snow growth across the LCL …2. yet very little change in MEAN vertical velocity across the LCL.

conclusion: snow growth must jump-start when the turbulent BL enters into cloud.

Page 17: Qun Miao Ningbo University Bart  Geerts University of Wyoming

WCR reflectivity (dBZ)

crest

LCL

Page 18: Qun Miao Ningbo University Bart  Geerts University of Wyoming

scatterplot where LWC > 0.05 g m-3, and the aircraft is within the BL

Liquid water in turbulent eddies within the BL

there is some positive correlation …snow must consume some of the droplets in the updrafts

Page 19: Qun Miao Ningbo University Bart  Geerts University of Wyoming

frequency-by-altitude displaynon-bright-band rain at CZD

Hei

ght,

MSL

(km

)

(Neiman et al., 2005, Mon. Wea. Rev.) profiling S-band radar data, time resolution 6 min (~4 km)

Is BL turbulence important also for the low-level growth by collision-coalescence in non-brightband

rain?

Page 20: Qun Miao Ningbo University Bart  Geerts University of Wyoming

low-level snow initiation?

2006-01-18

(a) Hallet-Mossop ice multiplication on rimed surfaces like trees: we have no evidence

Page 21: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Does blowing snow initiate glaciation in supercooled liquid orographic clouds?

fall speed removed

Page 22: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Blowing snow flights in ASCII (Jan-Feb 2012)

leg 5 along the Sierra Madre crest

KRWL *winds 30-40 kts during flight

sounding from BL2:deep well-mixed layerstrong windsT<0°C

Page 23: Qun Miao Ningbo University Bart  Geerts University of Wyoming

WCR reflectivity

WCR vertical velocity

WCL backscatter power

WCL depolarization ratio

blowing snow plumes??

high depol ratio suggests this is ice, not water

terrain outline, seen by radar & lidar

NW SE

Page 24: Qun Miao Ningbo University Bart  Geerts University of Wyoming

WCR reflectivity

WCR vertical velocity

WCL backscatter power

WCL depolarization ratio

Page 25: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Another blowing snow case,with a shallow stratus cloud deck upstream of mountain, cloud top temperature -14°C

leg 3 (along-wind)

Page 26: Qun Miao Ningbo University Bart  Geerts University of Wyoming

wind

WCR reflectivity

WCR vertical velocity

WCL backscatter power

WCL depolarization ratio

SW NE

cloud top (T~-12°C)

cloud must be thin because terrain can often be seen

DR is low at cloud top (droplets) and higher below (ice)

first snow(very light)

deep, turbulent BL

no seeding from aloft

Page 27: Qun Miao Ningbo University Bart  Geerts University of Wyoming

deep, turbulent BL, smooth wave motion aloft

windWCR reflectivity

WCL backscatter power

WCL depolarization ratio

SW NE

cloud top

WCR vertical velocity

terrain zoom-in (next slide)

Page 28: Qun Miao Ningbo University Bart  Geerts University of Wyoming

Depol Ratio is low at cloud top (droplets) and higher below (ice)

terrain

terrain

WCL backscatter power

WCL depolarization ratio

500

mcloud top

Page 29: Qun Miao Ningbo University Bart  Geerts University of Wyoming

conclusions• A turbulent BL drapes complex terrain.

– readily distinguishable from stratiform flow aloft

• FADs indicate rapid snow growth within the BL as the BL air rises through the cloud base.

• Shallow orographic clouds may be glaciated by the surface below.

• BL turbulence can strong (~convective updrafts)– may increase the fraction of accretional growth (riming).

Page 30: Qun Miao Ningbo University Bart  Geerts University of Wyoming

additional slides

Page 31: Qun Miao Ningbo University Bart  Geerts University of Wyoming

date 18 Jan 06

27-28 Jan 06

2 Feb 06

11 Feb 08

25 Feb 08

18 Feb 09

20 Feb 09

10 Mar 09

25 Mar 09

30 Mar 09

mean fallspeed at flight level (m s-1) 1.27 1.09 1.21 1.12 0.96 0.79 1.01 0.82 0.86 0.75

estimating hydrometeor terminal velocity

The FADs show the particle vertical motion.The fallspeed of snow is NOT removed.

gust probe: air vertical motion

WCR (mean close-gate below & above): particle vertical motion