Mixed&Layer&Heights&and&Aerosol&Products& … · 2013-01-08 · [email protected]" Author:...

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Mixed Layer Heights and Aerosol Products derived from the NASA LaRC Airborne High Spectral Resolu@on Lidar during the First DISCOVERAQ Field Mission Amy Jo Scarino 1,2 , Sharon Burton 2 , Richard Ferrare 2 , Chris Hostetler 2 , Mike Obland 2 , John Hair 2 , Ray Rogers 2 , Anthony Cook 2 , David Harper 2 , Arlindo DaSilva 3 , Brent Holben 3 , Ray Hoff 4 , Tim Berkoff 4 , Ruben Delgado 4 , Anne Thompson 5 , Joseph EvereIe 6 1 Science Systems and ApplicaLons, Inc., Hampton, VA USA 2 NASA Langley Research Center, Hampton, VA USA 3 NASA Goddard Space Flight Center, Greenbelt, MD USA 4 University of Maryland BalLmore County, BalLmore, MD USA 5 Pennsylvania State University, University Park, PA USA 6 Howard University, Washington, D. C. USA 2012 American Meteorological Society Annual Mee@ng 6 th Symposium on Lidar Atmospheric Applica@ons January 8, 2013

Transcript of Mixed&Layer&Heights&and&Aerosol&Products& … · 2013-01-08 · [email protected]" Author:...

Page 1: Mixed&Layer&Heights&and&Aerosol&Products& … · 2013-01-08 · amyjo.scarino@ssaihq.com" Author: Scarino, Amy Jo {Swanson} (LARC-E304)[SCIENCE SYSTEMS AND APPLICATIONS, INC] Created

Mixed  Layer  Heights  and  Aerosol  Products  derived  from  the  NASA  LaRC  Airborne  High  Spectral  Resolu@on  Lidar  during  the  First  

DISCOVER-­‐AQ  Field  Mission  Amy  Jo  Scarino1,2,  Sharon  Burton2,  Richard  Ferrare2,  Chris  Hostetler2,  Mike  Obland2,  John  

Hair2,  Ray  Rogers2,  Anthony  Cook2,  David  Harper2,  Arlindo  DaSilva3,  Brent  Holben3,    Ray  Hoff4,  Tim  Berkoff4,  Ruben  Delgado4,  Anne  Thompson5,  Joseph  EvereIe6  

   1Science  Systems  and  ApplicaLons,  Inc.,  Hampton,  VA  USA  

2NASA  Langley  Research  Center,  Hampton,  VA  USA  3NASA  Goddard  Space  Flight  Center,  Greenbelt,  MD  USA  

4University  of  Maryland  BalLmore  County,  BalLmore,  MD  USA  5Pennsylvania  State  University,  University  Park,  PA  USA  

6Howard  University,  Washington,  D.  C.  USA  

2012  American  Meteorological  Society  Annual  Mee@ng  6th  Symposium  on  Lidar  Atmospheric  Applica@ons  

January  8,  2013  

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NASA  Langley  Airborne    High  Spectral  Resolu@on  Lidar  (HSRL)  

DISCOVER-­‐AQ  (July  2011)  •  Deployed  on  NASA/LaRC  UC12  aircraU  •  Flight  al@tude  ~  9  km  •  Nadir  poin@ng  lidar  •  25  science  flights  (~100  science  hours)  •  Overflights  of  DISCOVER-­‐AQ  ground  sta@ons  and  AERONET  “DRAGON”  sites  

HSRL  Technique  •  Relies  on  spectral  separa@on  of  aerosol  and  

molecular  backsca`er  in  lidar  receiver  •  Independently  measures  aerosol  backsca`er,  

ex@nc@on,  and  op@cal  thickness  •  Internally  calibrated  independent  of  atmosphere  •  Provides  intensive  aerosol  parameters  to  help  

determine  aerosol  type  

HSRL  Aerosol  Data  Products  •  Backsca`er  coefficient  (532,  1064  nm)  •  Ex@nc@on  Coefficient  (532  nm)  •  Op@cal  depth  (532  nm)  •  Depolariza@on  (532,  1064  nm)  •  Mixed  Layer  (ML)  Height  from  aerosol  backsca`er  

gradients  

         AERONET  Sites            Ground  Sites  

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HSRL  data  used  to  find  height  of  Mixed  Layer  •  Mixed  Layer  (ML)  heights  derived  from  dayLme-­‐only  cloud-­‐screened  

aerosol  backscaIer  profiles  measured  by  the  airborne  HSRL;  ML  heights  are  a  good  proxy  for  PBL  heights  during  the  dayLme  

•  Automated  technique  uses  a  Haar  wavelet  covariance  transform  with  mulLple  wavelet  dilaLons  to  idenLfy  sharp  gradients  in  aerosol  backscaIer  at  the  top  of  the  ML  (adapted  from  Brooks,  JAOT,  2003)  

•  HSRL  ML  heights  combine  results  from  automated  algorithm  and  manual  inspecLon  of  HSRL  backscaIer  profiles  

•  Height  of  maximum  aerosol  gradient  also  idenLfied  to  provide  an  alternaLve  height  to  describe  the  depth  of  the  aerosol  layer  

•  These  heights  o`en  correspond  to  gradients  in  potenLal  temperature  

ML  Height  

Adapted  from  Stull  (1980),  Image  courtesy  Jerome  Fast  

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HSRL  ML  heights  over  land  and  water  •  ML  heights  are  generally  higher  over  land  than  over  water  (Chesapeake  Bay)  •  Height  of  maximum  aerosol  gradient  about  the  same  over  land  and  water  •  ML  height  and  height  of  maximum  aerosol  gradient  increased  during  the  day  

ML  Height   Height  of  max  aerosol  gradient  

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HSRL  ML  heights  compared  to    PBL  heights  from  MPL  

•  MPL  at  three  ground  sites  during  DISCOVER-­‐AQ:  Beltsville,  Edgewood  and  Fairhill  •  Comparisons  are  done  when  HSRL  was  within  2.5  km  of  the  ground  site  and  10  min  

from  the  MPL  measurement  •  Overall,  there  is  agreement  between  the  HSRL  ML  heights  and  MPL  PBL  heights  at  all  

sites  –  Outliers  are  most  likely  due  to  variability  in  the  locaLon  of  the  PBL  height  due  to  

clouds  and  geographic  locaLon,  as  well  as  differences  in  the  algorithm  deciding  what  is  the  ML  height  versus  the  maximum  aerosol  gradient  

Beltsville   Edgewood   Fairhill  

1:1  Line  Least-­‐squares  bisector  

1:1  Line  Least-­‐squares  bisector  

1:1  Line  Least-­‐squares  bisector  

R  =  0.863  Bisector  Slope  =  0.909  Bisector  Intercept  =  257  RMS  Error  =  309  m  Bias  Difference  =  152  m  

R  =  0.809  Bisector  Slope  =  0.986  Bisector  Intercept  =  35.8  RMS  Error  =  335  m  Bias  Difference  =  18.6  m  

R  =  0.789  Bisector  Slope  =  1.09  Bisector  Intercept  =  -­‐204  RMS  Error  =  357  m  Bias  Difference  =  96.2  m  

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HSRL  ML  heights  compared  the  PBL  heights    from  Ozonesonde  Poten@al  Temperature  Profile  

•  Ozonesondes  were  launched  ~2  Lmes  a  day  at  the  Beltsville  and  Edgewood  ground  sites  •  PBL  heights  are  determined  where  there  is  a  sharp  gradient  in  the  potenLal  temperature  

profile  and  when  inversion  criteria  are  met  (Heeer,  1980)  •  Comparison  is  done  when  HSRL  was  within  30  km  of  the  ground  site  and  30  min  from  

the  sonde  launch  Lme  

Heler  Inversion  Criteria  PBL  HSRL  ML  

Edgewood  Launch  Site  July  20  20:32  UTC  

1:1  Line  Least-­‐squares  bisector  

R  =  0.737  Bisector  Slope  =  1.06  Bisector  Intercept  =  -­‐186  RMS  Error  =  431  m  Bias  Difference  =  114  m  Number  Points  =  41  

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HSRL  and  AERONET  AOD  Comparisons  •  HSRL  0-­‐7  km  layer  AOD  (532  nm)  values  were  compared  with  column  AOD  

values  from  17  AERONET  “DRAGON”  sites  •  Comparison  is  done  when  HSRL  was  within  2.5  km  of  the  ground  site  and  10  

min  from  the  AERONET  measurement     •  HSRL  layer  AOD  values  were  highly  

correlated  with  AERONET  column  AOD  •  Small  (~0.03-­‐0.04)  offset  may  be  due  in  

part  (~0.02)  to  aerosol  above  7  km  from  June  2011  Nabra  volcano  erupLon  (Sawamura  et  al.,  2012,  ERL)  

1:1  Line  Least-­‐squares  bisector  

1:1  Line  Least-­‐squares  bisector  

R  =  0.971  Bisector  Slope  =  1.04  Bisector  Intercept  =  0.034  RMS  Error  =  0.064  Bias  Difference  =  0.043  Number  Points  =  329  

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AOD  above  and  within  ML  and    Maximum  Aerosol  Layer  

•  HSRL  measurements  are  used  to  determine  the  fracLon  of  AOD  in  0-­‐7  km  layer  that  is:  –  Below  and  above  the  ML  height  –  Below  and  above  the  height  of  

the  maximum  aerosol  gradient  

•  Before  about  local  noon  (~16  UTC),  more  AOD  above  ML  than  within  ML  

•  A`er  about  local  noon  (~16  UTC),  more  AOD  within  ML  than  above  ML  

•  About  70-­‐90%  of  AOD  was  below  the  height  of  the  maximum  aerosol  gradient  

•  Significant  increase  in  AOD  a`er  19  UTC  

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HSRL  ML  Heights  compared  to    GEOS-­‐5  ML  and  PBL  Heights  

HSRL-­‐1  

GEOS-­‐5  

•  Simulated  aerosol  backscaIer  from  the  GEOS-­‐5  model  along  the  HSRL  flight  tracks  was  processed  through  the  wavelet  covariance  transform  algorithm  to  produce  ML  heights  using  the  same  methodology  as  used  for  the  HSRL-­‐1  ML  heights  

•  On  average,  the  GEOS-­‐5  ML  heights  are  about  300-­‐500  m  higher  than  the  HSRL  ML  heights,  as  demonstrated  by  the  a`ernoon  flight  on  July  20th  and  also  in  the  scaIer  density  plot  that  compares  ML  heights  across  all  flights  during  the  mission    

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•  The  use  of  HSRL  ML  heights  to  evaluate  the  GEOS-­‐5  PBL  heights  for  the  July  2011  DISCOVER-­‐AQ  mission  led  to  the  discovery  of  issues  in  land  surface  characterizaLon  in  this  model  

•  IniLal  comparisons  indicated  that  the  model  PBL  heights  were  too  deep  (leU  figure);  further  invesLgaLon  revealed  that  this  was  due  to  overly  dry  land  surfaces  in  response  to  a  precipitaLon  deficit  in  spring    

•  Revising  the  land  surface  iniLal  condiLon  improved  not  only  the  PBL  heights  (right  figure)  but  also  led  to  beIer  heat  flux  raLos,  near-­‐surface  temperatures,  and  aerosol  verLcal  distribuLons  

HSRL  ML  Heights  compared  to    GEOS-­‐5  ML  and  PBL  Heights  

AUer  correc@on  Before  correc@on  

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•  ECMWF  model  results  and  HSRL  measurements  were  compared  along  the  King  Air  flight  tracks  for  14  field  missions  conducted  over  North  America  since  2006,  including  DISCOVER-­‐AQ  

•  PBL  heights  derived  using  the  parcel  li`ing  method  unLl  a  criLcal  Richardson  Number  is  reached  

•  AOD  from  HSRL  and  ECMWF,  is  used  to  determine  what  percentage  of  AOD  is  located  within  the  PBL  

•  While  ECMWF  PBL  heights  were  100-­‐200  m  higher  than  the  HSRL  ML  heights,  the  fracLon  of  AOD  within  the  PBL  was  about  the  same  for  ECMWF  and  HSRL  

HSRL  ML  Heights  compared  to    ECMWF  –MACC  PBL  Heights  

DISCOVER-­‐AQ  

HSRL  ML  Heights  (m,  AGL)   PBL  Height  (m,  AGL)  

ECMWF  PB

L  He

ights  (m,  A

GL)  

Thanks  to  Angela  Beneden  (ECMWF)  for  providing  the  model  data  to  us  

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Summary  •  PBL  height  is  a  key  parameter  for  simulaLng  climate  processes  and  assessing  model  simulaLon  of  aerosol  pollutant  concentraLons  and  transport  

•  ML  heights  from  airborne  lidar  are  a  good  proxy  for  the  dayLme  PBL  heights  and  are  useful  for  evaluaLng  PBL  heights  from  ground  site  instruments  and  from  numerical  weather  and  air  quality  models  

•  ML  heights  vary  with  land  vs.  water  and  Lme  of  day  •  FracLon  of  AOD  within  ML  varies  from  20-­‐80%  depending  on  Lme  •  FracLon  of  AOD  below  the  height  of  maximum  aerosol  gradient  varies  from  70-­‐90%  

•  HSRL  ML  heights  were  important  for  assessing  and  improving  GEOS-­‐5  model  •  Despite  good  agreement  in  general,  there  remain  differences  in  ML  and  PBL  heights  due  to  differences  in  definiLon  and  how  the  ML/PBL  are  determined  

Addi@onal  Studies  •  DISCOVER-­‐AQ  part  two  in  beginning  next  week  in  San  Joaquin  Valley,  CA  and  part  three  will  be  in  Houston,  TX  during  September  

•  Similar  ML/PBL  comparisons  will  be  done  for  the  San  Joaquin  Valley  and  Houston  regions  

•  WRF-­‐Chem  and  Lidar  ML  comparison  work  (Ray  Hoff)  •  Paper  is  in  the  preliminary  stages  for  the  DISCOVER-­‐AQ  work  in  the  DC/BalLmore  region    

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Contact  Info  Amy  Jo  Scarino  Science  Systems  and  ApplicaLons,  Inc.  NASA  Langley  Research  Center  Hampton,  VA    [email protected]  [email protected]