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Page 1: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

Analysis  of  TTL  wave  proper2es    and  rela2onships  to  cirrus  

 M.  Joan  Alexander1  Ji-­‐Eun  Kim2  

Thanks  to  the  ATTREX  Team  for  the  beau4ful  measurements  and  we  are  looking  forward  to  collabora4ons  on  

this  work.  

Page 2: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         TTL  Wave  Effects  on  Cirrus  Boehm  &  Verlinde  [2000]  •  Observa)ons  at  Nauru  

in  equatorial  Pacific  showed  Kelvin  wave  modula)on  of  cirrus.  

•  Implied  a  role  for  waves  in  dehydra)on  of  the  stratosphere.  

Cirrus  occurrence  above  15  km…    almost  exclusively  in  cold  phases  of  tropical  waves  

30-­‐day  Intensive  Observa2on  Period  Radiosonde  T  anomalies  &  Cirrus  from  Lidar  

Page 3: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         TTL  Wave  Effects  on  Cirrus  

How  important  are  these  higher  frequency  waves  to  cirrus  forma)on?  •  Regional  paIerns?  •  Seasonal  and  interannual  varia)ons?  

Wave  variance  near  the  cold  point  is  under-­‐represented  in  ERA-­‐Interim  

Kim  &  Alexander  [2013]  Western  Pacific  Radiosonde  Sites   §  Wave  periods  >  10  days  

(some  Kelvin  and  Rossby  waves)  are  fairly  well-­‐represented.    

§  Higher  frequencies  are  under-­‐represented.  

Page 4: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

GUAM  

Page 5: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

Flight  segments  along  constant  la)tude  ~6.5oN      

•  Total  length  ~2000km  

GUAM  

Page 6: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

12-­‐hourly  Radiosonde  Observa2on  Sites  

Chuuk  Koror   Ponape  Davado  

Page 7: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

Eastbound  w/dives  

“Wave  Flight”  

•  Dives  z  =  13.4  –  16.8km  •  CPL  shows  cirrus  layers  

~  12  –  16  km  

Page 8: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

Eastbound  w/dives  

“Wave  Flight”  

•  Dives  z  =  13.4  –  16.8km  •  CPL  shows  cirrus  layers  

~  12  –  16  km  

Page 9: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

Westbound  climbing  

“Wave  Flight”  

•  CPL  shows  cirrus  sloping  east-­‐to-­‐west  with  al)tude  

•  Slope  is  consistent  with  westward  wind  shear  or  westward  wave  propaga)on.  

Page 10: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  

Westbound  climbing  

“Wave  Flight”  

•  CPL  shows  cirrus  sloping  east-­‐to-­‐west  with  al)tude  

•  Slope  is  consistent  with  ver)cal  wind  shear  or  westward  wave  T’  

•  Drama)c  changes  on  )mescales  >  2hr  

+1  hr  +2.5  hr  +5  hr   -­‐20                                  -­‐10                                    0                                        10  Wind  (m/s)  

Al)tud

e  (km)  

   14              16

           18

             20  

U   V  

Page 11: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  Compute  Temperature  Anomalies  from  30-­‐day  2me-­‐mean  T  profile  

Mean  T  (K)  MERRA  

LONGITUDE  

ALTITU

DE  (K

M)  

Temperature  anomalies  reveal  fine-­‐scale  ver)cal  structure  ~1-­‐2  km  observed  by  MMS.  Horizontal  structure  >  1000km.  

Page 12: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  Similar  anomalies  also  seen  in  Zonal  and  Meridional  Wind  

Page 13: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  Rela2onships  between  FCDP  Par2cle  Counts  and  Temperature  Anomalies  

Page 14: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         ATTREX  Flight  6-­‐7  March  2014  Rela2onships  between  FCDP  Par2cle  Counts  and  Temperature  Anomalies  

600    500    400    300    200    100    0  

FCDP  Par)cle  Counts  

Cold  Anomalies  

Page 15: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  Anomalies  from  30-­‐day  Means   Filtered  to  retain  short  λZ  <  4  km  

Page 16: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  S-­‐Transform:  Time  History  of  Frequencies  of  Variability  

T  

U  

V  

Page 17: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  S-­‐Transform:  Time  History  of  Frequencies  of  Variability  

High  frequencies  (periods  ~  1day)  likely  influenced  by  missing  data  on  Day  +1  

T  

Page 18: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  S-­‐Transform:  Time  History  of  Frequencies  of  Variability  

•  Low  frequency    wave  (period    ~10  days)  is    Kelvin  wave.  

•  Temperature  anomaly  is  weak  on  flight  day.  

T  

Page 19: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  S-­‐Transform:  Time  History  of  Frequencies  of  Variability  in  the  TTL    

Wave  with  period  ~  3  days  present  on  the  flight  day  and  several  days  prior.  

U  

V  

T  

Page 20: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Radiosonde  Profiles  at  Chuuk  S-­‐Transform:  Cospectra  reveal  addi)onal  wave  proper)es  

Quadrature  in  (U,V),  (U,T),  and  (V,T)  reveal  the  3-­‐day  iner)a-­‐gravity  wave  is  propaga)ng  northwestward  rela)ve  to  the  wind.  

Page 21: Analysis(of(TTL(wave(proper2es(( andrelaonshipstocirrus · Analysis(of(TTL(wave(proper2es((andrelaonshipstocirrus M.(Joan(Alexander(1 JiEun Kim 2 Thanksto’the’ATTREX’Team’for’the’

         Conclusions  Analysis  of  the  “Wave  Flight”  at  7oN  on  6-­‐7  March  2014.  

 •  Evidence  that  cold  layers  ~1-­‐2  km  deep  due  to  waves  are  

influencing  cirrus  forma)on.  •  Both  10-­‐day  Kelvin  wave  and  3-­‐day  iner)a-­‐gravity  wave  signals  

with  ver)cal  wavelengths  <  4km  are  observed  at  Chuuk  in  days  leading  up  to  the  flight.  

•  Waves  of  such  fine  ver)cal  scale  are  not  resolved  in  reanalyses.  •  The  3-­‐day  wave  appears  to  be  the  dominant  signal  on  flight  day…  

an  observa)onal  first  for  iner)a-­‐gravity  waves  influencing  tropical  cirrus  forma)on?  

 Further  work  planned  to  compute  the  wave  horizontal  structure  u6lizing  addi6onal  radiosondes  and  MTP  observa6ons  and  hope  to  evaluate  wave  effects  on  dehydra6on.  


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