+ All Categories
Home > Documents > 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January...

1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January...

Date post: 28-Mar-2015
Category:
Upload: xavier-guthrie
View: 213 times
Download: 0 times
Share this document with a friend
Popular Tags:
8
1 ashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-O MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this release are based on analyses of IASI, AIRS, and AERI measurements in the region past the bandhead of the CO2 v3 band (~2385 cm-1): - Introduction of temperature dependence of carbon dioxide continuum absorption from 2386-2434 cm -1 from IASI measurements (E.J. Mlawer and V.H. Payne) - Modification of carbon dioxide continuum coefficients from 2000-3000 cm -1 from IASI and AERI (from ARM) measurements (E.J. Mlawer, V.H. Payne, and M.W. Shephard) - Modification of water vapor self continuum coefficients from 2000-3200 cm -1 from IASI and AIRS measurements; fit based on near-IR studies of Bicknell et al. (2006) and Fulghum and Tilleman (1991) (E.J. Mlawer and V.H. Payne)
Transcript
Page 1: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

1Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

MTCKD-2.5

Date: January 2010

MT_CKD_2.5 continuum modifications included in this release are based on analyses of IASI, AIRS, and AERI measurements in the region past the bandhead of the CO2 v3 band (~2385 cm-1):

- Introduction of temperature dependence of carbon dioxide continuum absorption from 2386-2434 cm-1 from IASI measurements (E.J. Mlawer and V.H. Payne)

- Modification of carbon dioxide continuum coefficients from 2000-3000 cm-1 from IASI and AERI (from ARM) measurements (E.J. Mlawer, V.H. Payne, and M.W. Shephard)

- Modification of water vapor self continuum coefficients from 2000-3200 cm-1 from IASI and AIRS measurements; fit based on near-IR studies of Bicknell et al. (2006) and Fulghum and Tilleman (1991) (E.J. Mlawer and V.H. Payne)

Page 2: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

2Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

MTCKD-2.5 vs MTCKD-1.3: Foreign

0 500 1000 1500 2000 2500 300010-27

10-26

10-25

10-24

10-23

10-22

10-21

cm-1

K,

cm

2 /mo

lec

/atm

H2O, MTCKD-1.0 (fore) H2O, MTCKD-1.3 (fore) H2O, MTCKD-2.5 (fore) -0.5

0.0

0.5

2 = NZ (18 all!) 2 = NG 1 15 For dimers opt.depth calculation in laboratory conditions cimulate homodginious path Z[km] P[mbar] T[K] H2O[ppmv] DIMER[ppmv] Keq=0.041 (M.Caro-Curtiss - 0.041) 0.000 .1013E+04 296.0 .100E-03 .100E+01 1.368 .1013E+04 296.0 .100E-03 .100E+01

( 1.3 - 1.0 ) / 1.0 ( 2.5 - 1.3 ) / 1.3

Page 3: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

3Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

MTCKD-2.5 vs MTCKD-1.3: Self

0 1000 2000 3000 400010-24

10-23

10-22

10-21

10-20

cm-1

K,

cm

2 /mo

lec

/atm

H2O, MTCKD-1.3 (self) H2O, MTCKD-2.5 (self)

0

2

4

6

8

0 ! M_RUN- Multi run flag: 0- one LBL run; 1- two LBL runs (second time uses lbl.in2) 0 0 ! ITR- Path's kind. (0-hor.; 1-vert.); IREDZ (1-RED.,0-NO) 0. 104. ! Z1, Z2 (Z2-IF ITR=1) - heights [KM] 1.00e-5 ! LEN - Length of horizontal path [KM]0. ! TETA - Zenith angle [GRAD]0. 20000. 0 ! FREQ1, FREQ2; Freq. units: 0-[CM-1], 1-[MKM], 2-[NM]25. 0.001 0 ! [CM-1] WINGs; H-MIN.SETKA (IF IAVTH=0, AUTOMAT. IF>0) 0.001 0 ! [CM-1] RES.STEP; ISRES=0 -USR, >0 H*ISRES; -1 -'FILTER' 2.0 0 ! [CM-1] OUT STEP; ISOUT: 0-USER, >0- OUT=H*ISOUT; 1 25. ! NG- No.of used gases; H2O_DIM >0 - H2O dimer HWHM instead of HCl (hit.ind.15) 1 2 7 15 4 5 6 7 22 4 6 15 3 7 4 5 6 7 15 9 11 12 10 ! NGAS(NG) - gases indexesC:HITRAN_200401_hit06_02_07_22_hit04+dimer2008-2003.par !hom_self_H2O.met 0 ! ISEL - SELECTION: 1 - ON, 0 - OFF 1.e-9 1.e-11 ! TAU0 TAU01 (IF ISEL=1) 1 1 ! CONTINUUM CKD24 1-ON, 0-OFF (H2O,CO2,O3,O2,N2); IONLY_CONT. 1-ON, 0-OFF 1 0 ! OUT: 1-OPT.DEPTH, 2-ABS., 3-TRANS.; IOPT_ML: 1-MULTILAYER OPT.DEPTH OUT 1 ! INTERPOLATION: 1-LINEAR; 2-KVADRAT. 3 ! READ LINES: 3-HITRAN-2004; 2-HITRAN96; 1-HITRAN91; 0-FROM LBL_ATL.DAT

2 = NZ (18 all!) 2 = NG 1 15 For dimers opt.depth calculation in laboratory conditions cimulate homodginious path Z[km] P[mbar] T[K] H2O[ppmv] DIMER[ppmv] Keq=0.041 (M.Caro-Curtiss - 0.041) 0.000 .200E+02 296.0 .100E+07 .100E+01 1.368 .200E+02 296.0 .100E+07 .100E+01

( 1.3 - 1.0 ) / 1.3 ( 2.5 - 1.3 ) / 1.3

Page 4: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

4Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

MTCKD-2.5 vs MTCKD-1.3: CO2 continuum

0 1000 2000 3000 4000 5000 6000 7000 800010-28

10-27

10-26

10-25

10-24

10-23

10-22

10-21

10-20

0 ! M_RUN- Multi run flag: 0- one LBL run; 1- two LBL runs (second time uses lbl.in2) 0 0 ! ITR- Path's kind. (0-hor.; 1-vert.); IREDZ (1-RED.,0-NO) 0.0 70. ! Z1, Z2 (Z2-IF ITR=1) - heights [KM] 1.0e-5 ! LEN - Length of horizontal path [KM]0. ! TETA - Zenith angle [GRAD]0. 20000. 0 ! FREQ1, FREQ2; Freq. units: 0-[CM-1], 1-[MKM], 2-[NM]25. 0.001 0 ! [CM-1] WINGs; H-MIN.SETKA (IF IAVTH=0, AUTOMAT. IF>0) 0.001 0 ! [CM-1] RES.STEP; ISRES=0 -USR, >0 H*ISRES; -1 -'FILTER' 2.0 0 ! [CM-1] OUT STEP; ISOUT: 0-USER, >0- OUT=H*ISOUT; 1 0. ! NG- No.of used gases; H2O_DIM >0 - H2O dimer HWHM instead of HCl (hit.ind.15) 22 ! NGAS(NG) - gases indexesC:\HITRAN\01-07_22_Hit08_(RS-fit_5300)_&_WD_2003-2008.par !hom_fore_H2O.met ! METEO (a30); '3DC_bec_LBL.met'- Multi-met regime! 0 ! ISEL - SELECTION: 1 - ON, 0 - OFF 1.e-9 1.e-11 ! TAU0 TAU01 (IF ISEL=1) 1 1 ! CONTINUUM CKD24 1-ON, 0-OFF (H2O,CO2,O3,O2,N2); IONLY_CONT. 1-ON, 0-OFF 1 0 ! OUT: 1-OPT.DEPTH, 2-ABS., 3-TRANS.; IOPT_ML: 1-MULTILAYER OPT.DEPTH OUT 1 ! INTERPOLATION: 1-LINEAR; 2-KVADRAT. 3 ! READ LINES: 3-HITRAN-2004; 2-HITRAN96; 1-HITRAN91; 0-FROM LBL_ATL.DAT 0 0 ! output: if 0- uniform out step, seted above (OUT STEP);

cm-1

K,

cm

2 /mo

lec

/atm

CO2, MTCKD-1.3 CO2, MTCKD-2.5

0

10

20

30

40

50

2 = NZ (18 all!) 2 = NG 1 15 For dimers opt.depth calculation in laboratory conditions cimulate homodginious path Z[km] P[mbar] T[K] H2O[ppmv] DIMER[ppmv] Keq=0.041 (M.Caro-Curtiss - 0.041) 0.000 .1013E+04 296.0 .100E-03 .100E+01 1.368 .1013E+04 296.0 .100E-03 .100E+01

( 2.5 - 1.3 ) / 1.3

Page 5: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

5Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

MTCKD-2.5 vs MTCKD-1.3: Self+Total

0 2000 4000 6000 8000 10000 1200010-5

10-4

10-3

10-2

10-1

100

101

102

cm-1

/1,2,3,7,22 gases; 0-70km, iao2+N2_rarefied.met/

0 ! M_RUN- Multi run flag: 0- one LBL run; 1- two LBL runs (second time uses lbl.in2) 1 0 ! ITR- Path's kind. (0-hor.; 1-vert.); IREDZ (1-RED.,0-NO) 0.0 70. ! Z1, Z2 (Z2-IF ITR=1) - heights [KM] 1.0e-5 ! LEN - Length of horizontal path [KM]0. ! TETA - Zenith angle [GRAD]0. 50000. 0 ! FREQ1, FREQ2; Freq. units: 0-[CM-1], 1-[MKM], 2-[NM]25. 0.001 0 ! [CM-1] WINGs; H-MIN.SETKA (IF IAVTH=0, AUTOMAT. IF>0) 0.001 0 ! [CM-1] RES.STEP; ISRES=0 -USR, >0 H*ISRES; -1 -'FILTER' 2.0 0 ! [CM-1] OUT STEP; ISOUT: 0-USER, >0- OUT=H*ISOUT; 5 0. ! NG- No.of used gases; H2O_DIM >0 - H2O dimer HWHM instead of HCl (hit.ind.15) 1 2 3 7 22 ! NGAS(NG) - gases indexesC:\HITRAN\01-07_22_Hit08_(RS-fit_5300)_&_WD_2003-2008.par !iao2+N2_rarefied.met ! METEO (a30); '3DC_bec_LBL.met'- Multi-met regime! 0 ! ISEL - SELECTION: 1 - ON, 0 - OFF 1.e-9 1.e-11 ! TAU0 TAU01 (IF ISEL=1) 1 1 ! CONTINUUM CKD24 1-ON, 0-OFF (H2O,CO2,O3,O2,N2); IONLY_CONT. 1-ON, 0-OFF 1 0 ! OUT: 1-OPT.DEPTH, 2-ABS., 3-TRANS.; IOPT_ML: 1-MULTILAYER OPT.DEPTH OUT 1 ! INTERPOLATION: 1-LINEAR; 2-KVADRAT. 3 ! READ LINES: 3-HITRAN-2004; 2-HITRAN96; 1-HITRAN91; 0-FROM LBL_ATL.DAT 0 0 ! output: if 0- uniform out step, seted above (OUT STEP);

MTCKD-1.3 MTCKD-2.5

Op

t. d

ep

th

0

5

10

15

(v2.5 - v.1.3) / v1.3

Page 6: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

6Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

Best spectral regions: TAFTS

100 150 200 2500

20

40

60

80 Up, Down & Net radiance at 11km, mW/(m2cm-1srad)

SZA=45o; Water_column=2.99 g/cm2

i ao2_H 2O from IC R C C M +N 2_40 .m e t:====================================================== 40 = N Z (32 a t a l l ) 14 = N G !!! N 2 added from ' us a . 1 2 3 4 5 6 7 8 9 10 11 12 15 22 (H 2O c o lum n=2 .99 g /c m 2)IO A -m ode l (S um m er, M id -la ti tude ) [P P M ]

Z[k m ] P [m ba r] T[K ] H 2O (3D C ) C O 2 O 3 N 2O C O C H 4 O 2 N O S O 2 N O 2 N H 3 H N O 3 D IM E R N 2

0 .00 .101E +04 292 .0 .188E +05 .333E +03 .205E -01 .281E +00 .468E +00 .148E +01 .207E +06 .711E -04 .839E -04 .372E -02 .987E -02 .987E -08 .148E +02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .04214 1 .00 .902E +03 288 .0 .138E +05 .331E +03 .326E -01 .281E +00 .126E +00 .148E +01 .207E +06 .188E -04 .967E -04 .269E -02 .987E -02 .987E -08 .874E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .04592 2 .00 .802E +03 283 .0 .959E +04 .328E +03 .390E -01 .281E +00 .126E +00 .148E +01 .207E +06 .200E -04 .110E -03 .195E -02 .987E -02 .987E -08 .470E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .05130 3 .00 .710E +03 278 .0 .622E +04 .325E +03 .450E -01 .281E +00 .126E +00 .148E +01 .207E +06 .213E -04 .122E -03 .141E -02 .987E -02 .987E -08 .220E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .05754 4 .00 .628E +03 272 .0 .397E +04 .322E +03 .497E -01 .281E +00 .126E +00 .148E +01 .207E +06 .226E -04 .135E -03 .102E -02 .987E -02 .987E -08 .649E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .06641 5 .00 .554E +03 266 .0 .270E +04 .320E +03 .538E -01 .281E +00 .126E +00 .148E +01 .207E +06 .241E -04 .148E -03 .736E -03 .987E -02 .987E -08 .308E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .07713 6 .00 .487E +03 260 .0 .159E +04 .317E +03 .578E -01 .281E +00 .111E +00 .148E +01 .207E +06 .256E -04 .129E -03 .532E -03 .987E -02 .987E -08 .110E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .09022 7 .00 .426E +03 253 .0 .905E +03 .314E +03 .614E -01 .281E +00 .980E -01 .148E +01 .207E +06 .273E -04 .111E -03 .385E -03 .987E -02 .987E -08 .377E -01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .10933 8 .00 .372E +03 246 .0 .635E +03 .311E +03 .666E -01 .281E +00 .864E -01 .148E +01 .207E +06 .291E -04 .918E -04 .278E -03 .987E -02 .987E -08 .198E -01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .13395 9 .00 .324E +03 239 .0 .397E +03 .318E +03 .731E -01 .281E +00 .761E -01 .148E +01 .207E +06 .306E -04 .730E -04 .201E -03 .987E -02 .987E -04 .837E -02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .16608 10 .00 .281E +03 233 .0 .238E +03 .324E +03 .955E -01 .281E +00 .670E -01 .148E +01 .207E +06 .644E -04 .543E -04 .360E -03 .987E -02 .326E -03 .317E -02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .20175 11 .00 .243E +03 227 .9 .823E +02 .331E +03 .144E +00 .281E +00 .594E -01 .149E +01 .207E +06 .135E -03 .523E -04 .788E -03 .987E -02 .778E -03 .390E -03 .780E +06 12 .00 .209E +03 223 .0 .286E +02 .336E +03 .195E +00 .281E +00 .520E -01 .148E +01 .207E +06 .285E -03 .503E -04 .115E -02 .987E -02 .118E -02 .482E -04 .780E +06 14 .00 .153E +03 218 .0 .461E +01 .330E +03 .290E +00 .281E +00 .404E -01 .137E +01 .207E +06 .126E -02 .464E -04 .140E -02 .987E -02 .158E -02 .110E -05 .780E +06 16 .00 .111E +03 216 .0 .445E +01 .325E +03 .542E +00 .281E +00 .313E -01 .126E +01 .207E +06 .290E -03 .424E -04 .170E -02 .987E -02 .188E -02 .806E -06 .780E +06 18 .00 .812E +02 217 .0 .429E +01 .319E +03 .119E +01 .236E +00 .243E -01 .116E +01 .207E +06 .412E -03 .385E -04 .207E -02 .987E -02 .207E -02 .527E -06 .780E +06 20 .00 .595E +02 220 .0 .432E +01 .324E +03 .213E +01 .197E +00 .189E -01 .107E +01 .207E +06 .584E -03 .345E -04 .252E -02 .987E -02 .296E -02 .350E -06 .780E +06 22 .00 .437E +02 222 .0 .604E +01 .329E +03 .316E +01 .165E +00 .146E -01 .989E +00 .207E +06 .828E -03 .306E -04 .306E -02 .987E -02 .415E -02 .466E -06 .780E +06 24 .00 .322E +02 225 .0 .778E +01 .334E +03 .436E +01 .138E +00 .118E -01 .913E +00 .207E +06 .117E -02 .266E -04 .372E -02 .987E -02 .592E -02 .511E -06 .780E +06 26 .00 .239E +02 228 .0 .985E +01 .339E +03 .538E +01 .116E +00 .140E -01 .842E +00 .207E +06 .167E -02 .227E -04 .452E -02 .987E -02 .347E -02 .547E -06 .780E +06 28 .00 .178E +02 231 .0 .114E +02 .344E +03 .614E +01 .970E -01 .162E -01 .777E +00 .207E +06 .236E -02 .188E -04 .550E -02 .987E -02 .299E -02 .493E -06 .780E +06 30 .00 .132E +02 234 .0 .133E +02 .341E +03 .665E +01 .809E -01 .184E -01 .717E +00 .207E +06 .335E -02 .148E -04 .669E -02 .987E -02 .257E -02 .450E -06 .780E +06 32 .50 .928E +01 240 .5 .129E +02 .329E +03 .781E +01 .461E -01 .211E -01 .648E +00 .207E +06 .516E -02 .127E -04 .852E -02 .987E -02 .747E -03 .243E -06 .780E +06 35 .00 .652E +01 247 .0 .125E +02 .317E +03 .866E +01 .263E -01 .238E -01 .586E +00 .207E +06 .804E -02 .109E -04 .109E -01 .987E -02 .217E -03 .131E -06 .780E +06 37 .50 .466E +01 253 .5 .125E +02 .305E +03 .763E +01 .150E -01 .265E -01 .530E +00 .207E +06 .124E -01 .109E -04 .144E -01 .987E -02 .146E -05 .742E -07 .780E +06 40 .00 .333E +01 260 .0 .119E +02 .294E +03 .672E +01 .856E -02 .292E -01 .479E +00 .207E +06 .193E -01 .109E -04 .178E -01 .987E -02 .987E -08 .420E -07 .780E +06 42 .50 .245E +01 267 .7 .109E +02 .280E +03 .472E +01 .482E -02 .316E -01 .428E +00 .207E +06 .293E -01 .109E -04 .178E -01 .987E -02 .987E -08 .221E -07 .780E +06 45 .00 .176E +01 273 .0 .103E +02 .273E +03 .340E +01 .278E -02 .346E -01 .392E +00 .207E +06 .462E -01 .109E -04 .178E -01 .987E -02 .987E -08 .119E -07 .780E +06 50 .00 .951E +00 276 .0 .100E +02 .254E +03 .287E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .566E -08 .780E +06 55 .00 .490E +00 272 .0 .889E +01 .254E +03 .217E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .254E -08 .780E +06 60 .00 .253E +00 264 .0 .826E +01 .254E +03 .160E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .138E -08 .780E +06 61 .67 .205E +00 256 .3 .693E +01 .254E +03 .151E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .900E -09 .780E +06 63 .33 .164E +00 248 .7 .590E +01 .254E +03 .144E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .700E -09 .780E +06 65 .00 .130E +00 241 .0 .508E +01 .254E +03 .139E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .517E -09 .780E +06 66 .67 .106E +00 233 .1 .368E +01 .254E +03 .130E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .300E -09 .780E +06 68 .33 .855E -01 225 .4 .272E +01 .254E +03 .118E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .100E -09 .780E +06 70 .00 .671E -01 218 .0 .206E +01 .254E +03 .104E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .967E -10 .780E +06 80 .00 .110E -01 215 .0 .238E +01 .254E +03 .223E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .237E -10 .780E +06 90 .00 .182E -02 213 .0 .286E +01 .254E +03 .103E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .614E -11 .780E +06100 .00 .300E -03 210 .0 .318E +01 .254E +03 .493E -01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .141E -11 .780E +06

!S U R F.A LB .: 0 .120

m y _d is o rt.in :-------------------------------------------------- 0 ! M _R U N - M u l ti -run flag : 0 - one D is o rt run ; 1 - tw o runs (2d run us es ' m y _d is o rt.in2 ' )H i t08_1 -7_22_M TC K D (noH 2O )_W D .D A T ! (a40 ) O P T.D E P TH fi l e to us eiao2_H 2O from IC R C C M +N 2_40 .m e t ! (a40 ) M e teo fi l e (.m e t/.a tm ) w as us ed to c rea te O P T.D E P TH fi l enew _k u ruc z _h r_0 .1c m -1 .da t ! (a40 ) S o la r fi l e w i th 2 c o lum ns : [c m -1 ] [W /(m 2* c m -1 )]1 640000 1 ! FIR S T and LA S T l ine from O P T.D E P TH fi l e to read ; and the S TE P - ' d Ifreq '

(d Ifreq=1 m eans ev e ry l i ne i s read , d Ifreq=2 - ev e ry s ec ond l ine e tc .)0 1 ! N res - N o . o f freq . S TE P S to av e rage fo r s pec tr. FLU X & IN TE N S . ou tpu t; N ou t_s tep - ou tpu t s tep 37 ! N o . o f a tm . lev e ls (from the bo ttom o f a tm os phe re ) to c a lc u la te5 5 ! Low er and U ppe r index o f a tm . lev e l (from the bo ttom ) be tw een w h ic h ou tpu t s pec tra l FLU X & IN TE N S ITIE S (>0 )

!* * * S e tup o f ae ros o l pa ram e te rs0 ! 1 -c oun t, 0 -no t c oun t ae ros o l4 ! N o f ae ros . s pec ies (up to 5 ) from ae ros o l -fi l e s (w i l l be readed one by one )3 2 3 3 ! N o f ae ros . g roups (m ax 3 ) and N o f s pec ies in eac h o f them (m ax 5 ) 2 3 1 2 4 1 2 4 ! Index es o f the c om ponen ts (from the ae ros o l fi l e ) fo r eac h g roup0 .05 0 .95 0 .7 0 .29 0 .01 0 .7 0 .29 0 .01 ! S pec ies v o lum e pe rc en tage in the eac h g roup [] 0 . 2 . 2 . 6 . 6 . 12 . ! [k m ] H e igh t range fo r eac h g roup 0 .025 0 .75 0 .0025 ! [k m -1 ] A bs . C oe ff. (0 .55m c r) fo r eac h g roup in the g iv en he ig th rangez 512 ! (a20 ) ae ros o l O p t. dep th fi l e1 61 61 ! FIR S T and LA S T l ine (w av e leng th ) to read from ae ros . fi l e and w ho le N o f w av e leng th the re

!* * * S e tup s om e inpu ts fo r D IS O R T0 ! us rtau : 1 - re tu rn rad ia tion a t us e r op t.dep ths , 0 - a t c om pu ted lev e ls0 ! us rang : 1 - re tu rn ou tpu t a t us e r po la r ang les (0 - a t c om pu ted ang les )4 ! ns tr - num ber o f c om p . po la r ang les (' s tream s ' ) ( num u = ns tr !)-1 .0 -0 .5 ! -0 .2113249 ! U M U (1 :ns tr/2 )- c os -s o f U S E R s po la r ang les (us ed on ly i f us rang=1 ) O n ly nega ti v e and in inc reas ing o rde r!!! 1 ! nph i - num ber o f az im u tha l ou tpu t ang les ; <=12 (us ed on ly i f ' on ly fl ' =0 )0 . ! ph i (nph i ) [deg .] - az im u th ang les to ou tpu t IN TE N S . (us ed on ly i f ' on ly fl ' =0 )0 .342 ! um u0 - c os ine o f s o la r po la r ang le * * * * * * * * * * c os (30 )=0 .866025 ; c os (45 )=0 .707 ; c os (50 )=0 .643 ; c os (70 )=0 .3420 . ! ph i0 - az im u th ang le o f inc iden t (s o la r!) beam (0 -360 deg r.)0 .0 ! fi s o t - In tens . o f top bounda ry IS O TR O P IC i l l um ina tion1 ! l am be r- (1 -true , 0 -fa ls e )1 ! on ly fl - (1 -true , 0 -fa ls e ). If ' 0 ' then U M U (), nph i , and ph i () m us t be s e t!1 ! p lnk - (1 P LA N K rad ia tion , 0 no p lank rad ia tion )16 ! nm om - num ber o f legand re po l inom ia l m om en ts1 ! Flug - fo r R ay legh s c a tte ring (1 -O n )

* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *Th is i s fo r Tom G ard ine r: from d i rec t s o la t fl ux obs e rv a tion (+ m ay be s om e s m a l l the rm a l flux in the s o la r s o l id ang le? )

lb l .i n :--------=----------------------------------- 0 ! M _R U N - M u l ti run flag : 0 - one LB L run ; 1 - tw o LB L runs (s ec ond tim e us es lb l .i n2 ) 1 0 ! ITR - P a th ' s k ind . (0 -ho r.; 1 -v e rt.); IR E D Z (1 -R E D .,0 -N O ) 0 .0 70 . ! Z1 , Z2 (Z2 -IF ITR =1 ) - he igh ts [K M ] 1 .00e -5 ! LE N - Leng th o f ho ri z on ta l pa th [K M ]0 . ! TE TA - Zen i th ang le [G R A D ]200 . 13000 . 0 ! FR E Q 1 , FR E Q 2; Freq . un i ts : 0 -[C M -1 ], 1 -[M K M ], 2 -[N M ]25 . 0 .001 0 ! [C M -1 ] W IN G s ; H -M IN .S E TK A (IF IA V TH =0 , A U TO M A T. IF>0 ) 0 .001 0 ! [C M -1 ] R E S .S TE P ; IS R E S =0 -U S R , >0 H * IS R E S ; -1 -' FILTE R ' 0 .02 0 ! [C M -1 ] O U T S TE P ; IS O U T: 0 -U S E R , >0 - O U T=H * IS O U T; 9 30 . ! N G - N o .o f us ed gas es ; H 2O _D IM >0 - H 2O d im er H W H M ins tead o f H C l (h i t.i nd .15 ) 1 2 3 4 5 6 7 15 22 8 9 10 11 22 4 6 15 3 7 4 5 6 7 15 9 11 12 10 ! N G A S (N G ) - gas es index esC :H ITR A N 01_H i t08_ (Fi t_5300 )_2 -7 ,22_& _W D _2003 -2008 .pa r !i ao2_H 2O from IC R C C M +N 2_40 .m e t hom _30m bH 2O .m e t ! M E TE O (a30 )! 0 ! IS E L - S E LE C TIO N : 1 - O N , 0 - O FF 1 .e -9 1 .e -11 ! TA U 0 TA U 01 (IF IS E L=1 ) 1 0 ! C O N TIN U U M C K D 24 1 -O N , 0 -O FF (H 2O ,C O 2 ,O 3 ,O 2 ,N 2 ); IO N LY _C O N T. 1 -O N , 0 -O FF 1 1 ! O U T: 1 -O P T.D E P TH , 2 -A B S ., 3 -TR A N S .; IO P T_M L: 1 -M U LTILA Y E R O P T.D E P TH O U T 1 ! IN TE R P O LA TIO N : 1 -L IN E A R ; 2 -K V A D R A T. 3 ! R E A D L IN E S : 3 -H ITR A N -2004 ; 2 -H ITR A N 96 ; 1 -H ITR A N 91 ; 0 -FR O M LB L_A TL .D A T 0 0 ! ou tpu t: i f 0 - un i fo rm ou t s tep , s e ted abov e (O U T S TE P );

DimerHWHM=30 cm-1; Keq=Curtiss

Ierror/IMTCKD

cm-1

Hit&CKD (Down) Hit&CKD (Up) Hit&CKD (NET) MTCKD contrib. (NET)

100 150 200 2500

1

2signal=signal*(1+0.05)+1.e-4 W/(m2cm-1srad)

dFerr / MTCKDcontr

Page 7: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

7Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

Best spectral regions: TAFTS

100 150 200 250

0.1

1

10

100 Up, Down & Net radiance at 4 km, mW/(m2cm-1srad)

iao2_H 2O from IC R C C M +N 2_40.m et:====================================================== 40 = N Z (32 at a l l ) 14 = N G !!! N 2 added from ' us a. 1 2 3 4 5 6 7 8 9 10 11 12 15 22 (H 2O c o lum n=2.99 g/c m 2)IO A -m odel (S um m er, M id-la ti tude) [P P M ]

Z[k m ] P [m bar] T[K ] H 2O (3D C ) C O 2 O 3 N 2O C O C H 4 O 2 N O S O 2 N O 2 N H 3 H N O 3 D IM E R N 2

0 .00 .101E +04 292.0 .188E +05 .333E +03 .205E -01 .281E +00 .468E +00 .148E +01 .207E +06 .711E -04 .839E -04 .372E -02 .987E -02 .987E -08 .148E +02 .780E +06 (M .C aro-C urtis s ) K eq=0.04214 1 .00 .902E +03 288.0 .138E +05 .331E +03 .326E -01 .281E +00 .126E +00 .148E +01 .207E +06 .188E -04 .967E -04 .269E -02 .987E -02 .987E -08 .874E +01 .780E +06 (M .C aro-C urtis s ) K eq=0.04592 2 .00 .802E +03 283.0 .959E +04 .328E +03 .390E -01 .281E +00 .126E +00 .148E +01 .207E +06 .200E -04 .110E -03 .195E -02 .987E -02 .987E -08 .470E +01 .780E +06 (M .C aro-C urtis s ) K eq=0.05130 3 .00 .710E +03 278.0 .622E +04 .325E +03 .450E -01 .281E +00 .126E +00 .148E +01 .207E +06 .213E -04 .122E -03 .141E -02 .987E -02 .987E -08 .220E +01 .780E +06 (M .C aro-C urtis s ) K eq=0.05754 4 .00 .628E +03 272.0 .397E +04 .322E +03 .497E -01 .281E +00 .126E +00 .148E +01 .207E +06 .226E -04 .135E -03 .102E -02 .987E -02 .987E -08 .649E +00 .780E +06 (M .C aro-C urtis s ) K eq=0.06641 5 .00 .554E +03 266.0 .270E +04 .320E +03 .538E -01 .281E +00 .126E +00 .148E +01 .207E +06 .241E -04 .148E -03 .736E -03 .987E -02 .987E -08 .308E +00 .780E +06 (M .C aro-C urtis s ) K eq=0.07713 6 .00 .487E +03 260.0 .159E +04 .317E +03 .578E -01 .281E +00 .111E +00 .148E +01 .207E +06 .256E -04 .129E -03 .532E -03 .987E -02 .987E -08 .110E +00 .780E +06 (M .C aro-C urtis s ) K eq=0.09022 7 .00 .426E +03 253.0 .905E +03 .314E +03 .614E -01 .281E +00 .980E -01 .148E +01 .207E +06 .273E -04 .111E -03 .385E -03 .987E -02 .987E -08 .377E -01 .780E +06 (M .C aro-C urtis s ) K eq=0.10933 8 .00 .372E +03 246.0 .635E +03 .311E +03 .666E -01 .281E +00 .864E -01 .148E +01 .207E +06 .291E -04 .918E -04 .278E -03 .987E -02 .987E -08 .198E -01 .780E +06 (M .C aro-C urtis s ) K eq=0.13395 9 .00 .324E +03 239.0 .397E +03 .318E +03 .731E -01 .281E +00 .761E -01 .148E +01 .207E +06 .306E -04 .730E -04 .201E -03 .987E -02 .987E -04 .837E -02 .780E +06 (M .C aro-C urtis s ) K eq=0.16608 10.00 .281E +03 233.0 .238E +03 .324E +03 .955E -01 .281E +00 .670E -01 .148E +01 .207E +06 .644E -04 .543E -04 .360E -03 .987E -02 .326E -03 .317E -02 .780E +06 (M .C aro-C urtis s ) K eq=0.20175 11.00 .243E +03 227.9 .823E +02 .331E +03 .144E +00 .281E +00 .594E -01 .149E +01 .207E +06 .135E -03 .523E -04 .788E -03 .987E -02 .778E -03 .390E -03 .780E +06 12.00 .209E +03 223.0 .286E +02 .336E +03 .195E +00 .281E +00 .520E -01 .148E +01 .207E +06 .285E -03 .503E -04 .115E -02 .987E -02 .118E -02 .482E -04 .780E +06 14.00 .153E +03 218.0 .461E +01 .330E +03 .290E +00 .281E +00 .404E -01 .137E +01 .207E +06 .126E -02 .464E -04 .140E -02 .987E -02 .158E -02 .110E -05 .780E +06 16.00 .111E +03 216.0 .445E +01 .325E +03 .542E +00 .281E +00 .313E -01 .126E +01 .207E +06 .290E -03 .424E -04 .170E -02 .987E -02 .188E -02 .806E -06 .780E +06 18.00 .812E +02 217.0 .429E +01 .319E +03 .119E +01 .236E +00 .243E -01 .116E +01 .207E +06 .412E -03 .385E -04 .207E -02 .987E -02 .207E -02 .527E -06 .780E +06 20.00 .595E +02 220.0 .432E +01 .324E +03 .213E +01 .197E +00 .189E -01 .107E +01 .207E +06 .584E -03 .345E -04 .252E -02 .987E -02 .296E -02 .350E -06 .780E +06 22.00 .437E +02 222.0 .604E +01 .329E +03 .316E +01 .165E +00 .146E -01 .989E +00 .207E +06 .828E -03 .306E -04 .306E -02 .987E -02 .415E -02 .466E -06 .780E +06 24.00 .322E +02 225.0 .778E +01 .334E +03 .436E +01 .138E +00 .118E -01 .913E +00 .207E +06 .117E -02 .266E -04 .372E -02 .987E -02 .592E -02 .511E -06 .780E +06 26.00 .239E +02 228.0 .985E +01 .339E +03 .538E +01 .116E +00 .140E -01 .842E +00 .207E +06 .167E -02 .227E -04 .452E -02 .987E -02 .347E -02 .547E -06 .780E +06 28.00 .178E +02 231.0 .114E +02 .344E +03 .614E +01 .970E -01 .162E -01 .777E +00 .207E +06 .236E -02 .188E -04 .550E -02 .987E -02 .299E -02 .493E -06 .780E +06 30.00 .132E +02 234.0 .133E +02 .341E +03 .665E +01 .809E -01 .184E -01 .717E +00 .207E +06 .335E -02 .148E -04 .669E -02 .987E -02 .257E -02 .450E -06 .780E +06 32.50 .928E +01 240.5 .129E +02 .329E +03 .781E +01 .461E -01 .211E -01 .648E +00 .207E +06 .516E -02 .127E -04 .852E -02 .987E -02 .747E -03 .243E -06 .780E +06 35.00 .652E +01 247.0 .125E +02 .317E +03 .866E +01 .263E -01 .238E -01 .586E +00 .207E +06 .804E -02 .109E -04 .109E -01 .987E -02 .217E -03 .131E -06 .780E +06 37.50 .466E +01 253.5 .125E +02 .305E +03 .763E +01 .150E -01 .265E -01 .530E +00 .207E +06 .124E -01 .109E -04 .144E -01 .987E -02 .146E -05 .742E -07 .780E +06 40.00 .333E +01 260.0 .119E +02 .294E +03 .672E +01 .856E -02 .292E -01 .479E +00 .207E +06 .193E -01 .109E -04 .178E -01 .987E -02 .987E -08 .420E -07 .780E +06 42.50 .245E +01 267.7 .109E +02 .280E +03 .472E +01 .482E -02 .316E -01 .428E +00 .207E +06 .293E -01 .109E -04 .178E -01 .987E -02 .987E -08 .221E -07 .780E +06 45.00 .176E +01 273.0 .103E +02 .273E +03 .340E +01 .278E -02 .346E -01 .392E +00 .207E +06 .462E -01 .109E -04 .178E -01 .987E -02 .987E -08 .119E -07 .780E +06 50.00 .951E +00 276.0 .100E +02 .254E +03 .287E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .566E -08 .780E +06 55.00 .490E +00 272.0 .889E +01 .254E +03 .217E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .254E -08 .780E +06 60.00 .253E +00 264.0 .826E +01 .254E +03 .160E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .138E -08 .780E +06 61.67 .205E +00 256.3 .693E +01 .254E +03 .151E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .900E -09 .780E +06 63.33 .164E +00 248.7 .590E +01 .254E +03 .144E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .700E -09 .780E +06 65.00 .130E +00 241.0 .508E +01 .254E +03 .139E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .517E -09 .780E +06 66.67 .106E +00 233.1 .368E +01 .254E +03 .130E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .300E -09 .780E +06 68.33 .855E -01 225.4 .272E +01 .254E +03 .118E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .100E -09 .780E +06 70.00 .671E -01 218.0 .206E +01 .254E +03 .104E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .967E -10 .780E +06 80.00 .110E -01 215.0 .238E +01 .254E +03 .223E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .237E -10 .780E +06 90.00 .182E -02 213.0 .286E +01 .254E +03 .103E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .614E -11 .780E +06100.00 .300E -03 210.0 .318E +01 .254E +03 .493E -01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .141E -11 .780E +06

!S U R F.A LB .: 0 .120

m y _dis ort.in :-------------------------------------------------- 0 ! M _R U N - M ul ti -run flag: 0- one D is ort run; 1- tw o runs (2d run us es ' m y _dis ort.in2 ' )H i t08_1-7_22_M TC K D (noH 2O )_W D .D A T ! (a40) O P T.D E P TH fi le to us eiao2_H 2O from IC R C C M +N 2_40.m et ! (a40) M eteo fi le (.m et/.a tm ) w as us ed to c reate O P T.D E P TH fi lenew _k uruc z _hr_0.1c m -1.dat ! (a40) S olar fi le w i th 2 c o lum ns : [c m -1] [W /(m 2* c m -1)]1 640000 1 ! FIR S T and LA S T l ine from O P T.D E P TH fi le to read; and the S TE P - ' d Ifreq '

(d Ifreq=1 m eans ev ery l ine is read, d Ifreq=2 - ev ery s ec ond l ine e tc .)0 1 ! N res - N o. o f freq. S TE P S to av erage for s pec tr. FLU X & IN TE N S . output; N out_s tep - output s tep 37 ! N o. o f a tm . lev e ls (from the bottom of a tm os phere) to c a lc u la te5 5 ! Low er and U pper index of a tm . lev e l (from the bottom ) betw een w hic h output s pec tra l FLU X & IN TE N S ITIE S (>0)

!* * * S etup of aeros ol param eters0 ! 1-c ount, 0-not c ount aeros ol4 ! N of aeros . s pec ies (up to 5) from aeros ol -fi les (w i l l be readed one by one)3 2 3 3 ! N of aeros . groups (m ax 3) and N of s pec ies in eac h of them (m ax 5) 2 3 1 2 4 1 2 4 ! Index es of the c om ponents (from the aeros ol fi le ) for eac h group0.05 0.95 0 .7 0 .29 0.01 0 .7 0 .29 0.01 ! S pec ies v o lum e perc entage in the eac h group [] 0 . 2 . 2 . 6 . 6 . 12. ! [k m ] H eight range for eac h group 0 .025 0 .75 0 .0025 ! [k m -1] A bs . C oeff. (0 .55m c r) for eac h group in the g iv en he ig th rangez 512 ! (a20) aeros ol O pt. depth fi le1 61 61 ! FIR S T and LA S T l ine (w av elength) to read from aeros . fi le and w hole N of w av elength there

!* * * S etup s om e inputs for D IS O R T0 ! us rtau: 1- re turn rad ia tion at us er opt.depths , 0- a t c om puted lev e ls0 ! us rang: 1- re turn output a t us er po lar angles (0- a t c om puted angles )4 ! ns tr - num ber o f c om p. po lar angles (' s tream s ' ) ( num u = ns tr !)-1 .0 -0 .5 ! -0 .2113249 ! U M U (1:ns tr/2)- c os -s o f U S E R s polar angles (us ed on ly i f us rang=1) O nly negativ e and in inc reas ing order!!! 1 ! nph i - num ber o f az im utha l output angles ; <=12 (us ed on ly i f ' on ly fl ' =0)0. ! ph i (nphi ) [deg.] - az im uth angles to output IN TE N S . (us ed on ly i f ' on ly fl ' =0)0.342 ! um u0 - c os ine of s o lar po lar angle * * * * * * * * * * c os (30)=0.866025; c os (45)=0.707; c os (50)=0.643; c os (70)=0.3420. ! ph i0 - az im uth angle o f inc ident (s o lar!) beam (0-360 degr.)0 .0 ! fis o t - In tens . o f top boundary IS O TR O P IC i l lum ination1 ! lam ber- (1-true, 0-fa ls e)1 ! on ly fl - (1-true, 0-fa ls e). If ' 0 ' then U M U (), nphi , and ph i () m us t be s et!1 ! p lnk - (1 P LA N K rad ia tion, 0 no p lank rad ia tion)16 ! nm om - num ber o f legandre po l inom ia l m om ents1 ! Flug - for R ay legh s c attering (1-O n)

* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *This is for Tom G ard iner: from d i rec t s o la t flux obs erv ation (+ m ay be s om e s m al l therm al flux in the s o lar s o l id angle?)

lb l .in :--------=----------------------------------- 0 ! M _R U N - M ul ti run flag: 0- one LB L run; 1- tw o LB L runs (s ec ond tim e us es lb l .in2) 1 0 ! ITR - P ath ' s k ind. (0-hor.; 1-v ert.); IR E D Z (1-R E D .,0-N O ) 0.0 70. ! Z1, Z2 (Z2-IF ITR =1) - he ights [K M ] 1 .00e-5 ! LE N - Length o f horiz onta l path [K M ]0. ! TE TA - Zeni th angle [G R A D ]200. 13000. 0 ! FR E Q 1, FR E Q 2; Freq. un i ts : 0-[C M -1], 1-[M K M ], 2-[N M ]25. 0 .001 0 ! [C M -1] W IN G s ; H -M IN .S E TK A (IF IA V TH =0, A U TO M A T. IF>0) 0 .001 0 ! [C M -1] R E S .S TE P ; IS R E S =0 -U S R , >0 H * IS R E S ; -1 -' FILTE R ' 0 .02 0 ! [C M -1] O U T S TE P ; IS O U T: 0-U S E R , >0- O U T=H * IS O U T; 9 30. ! N G - N o.of us ed gas es ; H 2O _D IM >0 - H 2O d im er H W H M ins tead of H C l (h i t.ind.15) 1 2 3 4 5 6 7 15 22 8 9 10 11 22 4 6 15 3 7 4 5 6 7 15 9 11 12 10 ! N G A S (N G ) - gas es index esC :H ITR A N 01_H i t08_(Fi t_5300)_2-7,22_& _W D _2003-2008.par !iao2_H 2O from IC R C C M +N 2_40.m et hom _30m bH 2O .m et ! M E TE O (a30)! 0 ! IS E L - S E LE C TIO N : 1 - O N , 0 - O FF 1.e-9 1 .e-11 ! TA U 0 TA U 01 (IF IS E L=1) 1 0 ! C O N TIN U U M C K D 24 1-O N , 0-O FF (H 2O ,C O 2,O 3,O 2,N 2); IO N LY _C O N T. 1-O N , 0-O FF 1 1 ! O U T: 1-O P T.D E P TH , 2-A B S ., 3-TR A N S .; IO P T_M L: 1-M U LTILA Y E R O P T.D E P TH O U T 1 ! IN TE R P O LA TIO N : 1-LIN E A R ; 2-K V A D R A T. 3 ! R E A D LIN E S : 3-H ITR A N -2004; 2-H ITR A N 96; 1-H ITR A N 91; 0-FR O M LB L_A TL.D A T 0 0 ! output: i f 0- un i form out s tep, s eted abov e (O U T S TE P );

DimerHWHM=30 cm-1; Keq=Curtiss

Ierror/IMTCKD

cm-1

Hit&CKD (Down) Hit&CKD (Up) Hit&CKD (NET) MTCKD contrib. (NET)

100 150 200 2500

1

2

3 signal=signal*(1+0.05)+1.e-4 W/(m2cm-1srad)

SZA=45o; Water_column=2.99 g/cm2

dFerr / MTCKDcontr

Page 8: 1 Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office MTCKD-2.5 Date: January 2010 MT_CKD_2.5 continuum modifications included in this.

8Igor Ptashnik (Reading) 29 April, 2010 Field CAVIAR meeting, Met-Office

Best spectral regions: TAFTS

100 150 200 2500

20

40

60

80

i ao2_H 2O from IC R C C M +N 2_40 .m e t:====================================================== 40 = N Z (32 a t a l l ) 14 = N G !!! N 2 added from ' us a . 1 2 3 4 5 6 7 8 9 10 11 12 15 22 (H 2O c o lum n=2 .99 g /c m 2)IO A -m ode l (S um m er, M id -la ti tude ) [P P M ]

Z[k m ] P [m ba r] T[K ] H 2O (3D C ) C O 2 O 3 N 2O C O C H 4 O 2 N O S O 2 N O 2 N H 3 H N O 3 D IM E R N 2

0 .00 .101E +04 292 .0 .188E +05 .333E +03 .205E -01 .281E +00 .468E +00 .148E +01 .207E +06 .711E -04 .839E -04 .372E -02 .987E -02 .987E -08 .148E +02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .04214 1 .00 .902E +03 288 .0 .138E +05 .331E +03 .326E -01 .281E +00 .126E +00 .148E +01 .207E +06 .188E -04 .967E -04 .269E -02 .987E -02 .987E -08 .874E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .04592 2 .00 .802E +03 283 .0 .959E +04 .328E +03 .390E -01 .281E +00 .126E +00 .148E +01 .207E +06 .200E -04 .110E -03 .195E -02 .987E -02 .987E -08 .470E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .05130 3 .00 .710E +03 278 .0 .622E +04 .325E +03 .450E -01 .281E +00 .126E +00 .148E +01 .207E +06 .213E -04 .122E -03 .141E -02 .987E -02 .987E -08 .220E +01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .05754 4 .00 .628E +03 272 .0 .397E +04 .322E +03 .497E -01 .281E +00 .126E +00 .148E +01 .207E +06 .226E -04 .135E -03 .102E -02 .987E -02 .987E -08 .649E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .06641 5 .00 .554E +03 266 .0 .270E +04 .320E +03 .538E -01 .281E +00 .126E +00 .148E +01 .207E +06 .241E -04 .148E -03 .736E -03 .987E -02 .987E -08 .308E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .07713 6 .00 .487E +03 260 .0 .159E +04 .317E +03 .578E -01 .281E +00 .111E +00 .148E +01 .207E +06 .256E -04 .129E -03 .532E -03 .987E -02 .987E -08 .110E +00 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .09022 7 .00 .426E +03 253 .0 .905E +03 .314E +03 .614E -01 .281E +00 .980E -01 .148E +01 .207E +06 .273E -04 .111E -03 .385E -03 .987E -02 .987E -08 .377E -01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .10933 8 .00 .372E +03 246 .0 .635E +03 .311E +03 .666E -01 .281E +00 .864E -01 .148E +01 .207E +06 .291E -04 .918E -04 .278E -03 .987E -02 .987E -08 .198E -01 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .13395 9 .00 .324E +03 239 .0 .397E +03 .318E +03 .731E -01 .281E +00 .761E -01 .148E +01 .207E +06 .306E -04 .730E -04 .201E -03 .987E -02 .987E -04 .837E -02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .16608 10 .00 .281E +03 233 .0 .238E +03 .324E +03 .955E -01 .281E +00 .670E -01 .148E +01 .207E +06 .644E -04 .543E -04 .360E -03 .987E -02 .326E -03 .317E -02 .780E +06 (M .C a ro -C u rti s s ) K eq=0 .20175 11 .00 .243E +03 227 .9 .823E +02 .331E +03 .144E +00 .281E +00 .594E -01 .149E +01 .207E +06 .135E -03 .523E -04 .788E -03 .987E -02 .778E -03 .390E -03 .780E +06 12 .00 .209E +03 223 .0 .286E +02 .336E +03 .195E +00 .281E +00 .520E -01 .148E +01 .207E +06 .285E -03 .503E -04 .115E -02 .987E -02 .118E -02 .482E -04 .780E +06 14 .00 .153E +03 218 .0 .461E +01 .330E +03 .290E +00 .281E +00 .404E -01 .137E +01 .207E +06 .126E -02 .464E -04 .140E -02 .987E -02 .158E -02 .110E -05 .780E +06 16 .00 .111E +03 216 .0 .445E +01 .325E +03 .542E +00 .281E +00 .313E -01 .126E +01 .207E +06 .290E -03 .424E -04 .170E -02 .987E -02 .188E -02 .806E -06 .780E +06 18 .00 .812E +02 217 .0 .429E +01 .319E +03 .119E +01 .236E +00 .243E -01 .116E +01 .207E +06 .412E -03 .385E -04 .207E -02 .987E -02 .207E -02 .527E -06 .780E +06 20 .00 .595E +02 220 .0 .432E +01 .324E +03 .213E +01 .197E +00 .189E -01 .107E +01 .207E +06 .584E -03 .345E -04 .252E -02 .987E -02 .296E -02 .350E -06 .780E +06 22 .00 .437E +02 222 .0 .604E +01 .329E +03 .316E +01 .165E +00 .146E -01 .989E +00 .207E +06 .828E -03 .306E -04 .306E -02 .987E -02 .415E -02 .466E -06 .780E +06 24 .00 .322E +02 225 .0 .778E +01 .334E +03 .436E +01 .138E +00 .118E -01 .913E +00 .207E +06 .117E -02 .266E -04 .372E -02 .987E -02 .592E -02 .511E -06 .780E +06 26 .00 .239E +02 228 .0 .985E +01 .339E +03 .538E +01 .116E +00 .140E -01 .842E +00 .207E +06 .167E -02 .227E -04 .452E -02 .987E -02 .347E -02 .547E -06 .780E +06 28 .00 .178E +02 231 .0 .114E +02 .344E +03 .614E +01 .970E -01 .162E -01 .777E +00 .207E +06 .236E -02 .188E -04 .550E -02 .987E -02 .299E -02 .493E -06 .780E +06 30 .00 .132E +02 234 .0 .133E +02 .341E +03 .665E +01 .809E -01 .184E -01 .717E +00 .207E +06 .335E -02 .148E -04 .669E -02 .987E -02 .257E -02 .450E -06 .780E +06 32 .50 .928E +01 240 .5 .129E +02 .329E +03 .781E +01 .461E -01 .211E -01 .648E +00 .207E +06 .516E -02 .127E -04 .852E -02 .987E -02 .747E -03 .243E -06 .780E +06 35 .00 .652E +01 247 .0 .125E +02 .317E +03 .866E +01 .263E -01 .238E -01 .586E +00 .207E +06 .804E -02 .109E -04 .109E -01 .987E -02 .217E -03 .131E -06 .780E +06 37 .50 .466E +01 253 .5 .125E +02 .305E +03 .763E +01 .150E -01 .265E -01 .530E +00 .207E +06 .124E -01 .109E -04 .144E -01 .987E -02 .146E -05 .742E -07 .780E +06 40 .00 .333E +01 260 .0 .119E +02 .294E +03 .672E +01 .856E -02 .292E -01 .479E +00 .207E +06 .193E -01 .109E -04 .178E -01 .987E -02 .987E -08 .420E -07 .780E +06 42 .50 .245E +01 267 .7 .109E +02 .280E +03 .472E +01 .482E -02 .316E -01 .428E +00 .207E +06 .293E -01 .109E -04 .178E -01 .987E -02 .987E -08 .221E -07 .780E +06 45 .00 .176E +01 273 .0 .103E +02 .273E +03 .340E +01 .278E -02 .346E -01 .392E +00 .207E +06 .462E -01 .109E -04 .178E -01 .987E -02 .987E -08 .119E -07 .780E +06 50 .00 .951E +00 276 .0 .100E +02 .254E +03 .287E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .566E -08 .780E +06 55 .00 .490E +00 272 .0 .889E +01 .254E +03 .217E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .254E -08 .780E +06 60 .00 .253E +00 264 .0 .826E +01 .254E +03 .160E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .138E -08 .780E +06 61 .67 .205E +00 256 .3 .693E +01 .254E +03 .151E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .900E -09 .780E +06 63 .33 .164E +00 248 .7 .590E +01 .254E +03 .144E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .700E -09 .780E +06 65 .00 .130E +00 241 .0 .508E +01 .254E +03 .139E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .517E -09 .780E +06 66 .67 .106E +00 233 .1 .368E +01 .254E +03 .130E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .300E -09 .780E +06 68 .33 .855E -01 225 .4 .272E +01 .254E +03 .118E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .100E -09 .780E +06 70 .00 .671E -01 218 .0 .206E +01 .254E +03 .104E +01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .967E -10 .780E +06 80 .00 .110E -01 215 .0 .238E +01 .254E +03 .223E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .237E -10 .780E +06 90 .00 .182E -02 213 .0 .286E +01 .254E +03 .103E +00 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .614E -11 .780E +06100 .00 .300E -03 210 .0 .318E +01 .254E +03 .493E -01 .905E -03 .401E -01 .479E +00 .207E +06 .111E +00 .109E -04 .178E -01 .987E -02 .987E -08 .141E -11 .780E +06

!S U R F.A LB .: 0 .120

m y _d is o rt.i n :-------------------------------------------------- 0 ! M _R U N - M u l ti -run flag : 0 - one D is o rt run ; 1 - tw o runs (2d run us es ' m y _d is o rt.i n2 ' )H i t08_1 -7_22_M TC K D (noH 2O )_W D .D A T ! (a40 ) O P T.D E P TH fi l e to us eiao2_H 2O from IC R C C M +N 2_40 .m e t ! (a40 ) M e teo fi l e (.m e t/.a tm ) w as us ed to c rea te O P T.D E P TH fi l enew _k u ruc z _h r_0 .1c m -1 .da t ! (a40 ) S o la r fi l e w i th 2 c o lum ns : [c m -1 ] [W /(m 2* c m -1 )]1 640000 1 ! FIR S T and LA S T l ine from O P T.D E P TH fi l e to read ; and the S TE P - ' d Ifreq '

(d Ifreq=1 m eans ev e ry l i ne i s read , d Ifreq=2 - ev e ry s ec ond l i ne e tc .)0 1 ! N res - N o . o f freq . S TE P S to av e rage fo r s pec tr. FLU X & IN TE N S . ou tpu t; N ou t_s tep - ou tpu t s tep 37 ! N o . o f a tm . lev e ls (from the bo ttom o f a tm os phe re ) to c a lc u la te5 5 ! Low er and U ppe r index o f a tm . lev e l (from the bo ttom ) be tw een w h ic h ou tpu t s pec tra l FLU X & IN TE N S ITIE S (>0 )

!* * * S e tup o f ae ros o l pa ram e te rs0 ! 1 -c oun t, 0 -no t c oun t ae ros o l4 ! N o f ae ros . s pec ies (up to 5 ) from ae ros o l -fi l e s (w i l l be readed one by one )3 2 3 3 ! N o f ae ros . g roups (m ax 3 ) and N o f s pec ies in eac h o f them (m ax 5 ) 2 3 1 2 4 1 2 4 ! Index es o f the c om ponen ts (from the ae ros o l fi l e ) fo r eac h g roup0 .05 0 .95 0 .7 0 .29 0 .01 0 .7 0 .29 0 .01 ! S pec ies v o lum e pe rc en tage in the eac h g roup [] 0 . 2 . 2 . 6 . 6 . 12 . ! [k m ] H e igh t range fo r eac h g roup 0 .025 0 .75 0 .0025 ! [k m -1 ] A bs . C oe ff. (0 .55m c r) fo r eac h g roup in the g iv en he ig th rangez 512 ! (a20 ) ae ros o l O p t. dep th fi l e1 61 61 ! FIR S T and LA S T l ine (w av e leng th ) to read from ae ros . fi l e and w ho le N o f w av e leng th the re

!* * * S e tup s om e inpu ts fo r D IS O R T0 ! us rtau : 1 - re tu rn rad ia tion a t us e r op t.dep ths , 0 - a t c om pu ted lev e ls0 ! us rang : 1 - re tu rn ou tpu t a t us e r po la r ang les (0 - a t c om pu ted ang les )4 ! ns tr - num ber o f c om p . po la r ang les (' s tream s ' ) ( num u = ns tr !)-1 .0 -0 .5 ! -0 .2113249 ! U M U (1 :ns tr/2 )- c os -s o f U S E R s po la r ang les (us ed on ly i f us rang=1 ) O n ly nega ti v e and in inc reas ing o rde r!!! 1 ! nph i - num ber o f az im u tha l ou tpu t ang les ; <=12 (us ed on ly i f ' on ly fl ' =0 )0 . ! ph i (nph i ) [deg .] - az im u th ang les to ou tpu t IN TE N S . (us ed on ly i f ' on ly fl ' =0 )0 .342 ! um u0 - c os ine o f s o la r po la r ang le * * * * * * * * * * c os (30 )=0 .866025 ; c os (45 )=0 .707 ; c os (50 )=0 .643 ; c os (70 )=0 .3420 . ! ph i0 - az im u th ang le o f inc iden t (s o la r!) beam (0 -360 deg r.)0 .0 ! fi s o t - In tens . o f top bounda ry IS O TR O P IC i l l um ina tion1 ! l am be r- (1 -true , 0 -fa ls e )1 ! on ly fl - (1 -true , 0 -fa ls e ). If ' 0 ' then U M U (), nph i , and ph i () m us t be s e t!1 ! p lnk - (1 P LA N K rad ia tion , 0 no p lank rad ia tion )16 ! nm om - num ber o f legand re po l inom ia l m om en ts1 ! Flug - fo r R ay legh s c a tte ring (1 -O n )

* * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * *Th is i s fo r Tom G ard ine r: from d i rec t s o la t fl u x obs e rv a tion (+ m ay be s om e s m a l l the rm a l fl u x in the s o la r s o l id ang le? )

lb l .i n :--------=----------------------------------- 0 ! M _R U N - M u l ti run flag : 0 - one LB L run ; 1 - tw o LB L runs (s ec ond tim e us es lb l .i n2 ) 1 0 ! ITR - P a th ' s k ind . (0 -ho r.; 1 -v e rt.); IR E D Z (1 -R E D .,0 -N O ) 0 .0 70 . ! Z1 , Z2 (Z2 -IF ITR =1 ) - he igh ts [K M ] 1 .00e -5 ! LE N - Leng th o f ho ri z on ta l pa th [K M ]0 . ! TE TA - Zen i th ang le [G R A D ]200 . 13000 . 0 ! FR E Q 1 , FR E Q 2 ; Freq . un i ts : 0 -[C M -1 ], 1 -[M K M ], 2 -[N M ]25 . 0 .001 0 ! [C M -1 ] W IN G s ; H -M IN .S E TK A (IF IA V TH =0 , A U TO M A T. IF>0 ) 0 .001 0 ! [C M -1 ] R E S .S TE P ; IS R E S =0 -U S R , >0 H * IS R E S ; -1 -' FILTE R ' 0 .02 0 ! [C M -1 ] O U T S TE P ; IS O U T: 0 -U S E R , >0 - O U T=H * IS O U T; 9 30 . ! N G - N o .o f us ed gas es ; H 2O _D IM >0 - H 2O d im e r H W H M ins tead o f H C l (h i t.i nd .15 ) 1 2 3 4 5 6 7 15 22 8 9 10 11 22 4 6 15 3 7 4 5 6 7 15 9 11 12 10 ! N G A S (N G ) - gas es index esC :H ITR A N 01_H i t08_ (Fi t_5300 )_2 -7 ,22_& _W D _2003 -2008 .pa r !i ao2_H 2O from IC R C C M +N 2_40 .m e t hom _30m bH 2O .m e t ! M E TE O (a30 )! 0 ! IS E L - S E LE C TIO N : 1 - O N , 0 - O FF 1 .e -9 1 .e -11 ! TA U 0 TA U 01 (IF IS E L=1 ) 1 0 ! C O N TIN U U M C K D 24 1 -O N , 0 -O FF (H 2O ,C O 2 ,O 3 ,O 2 ,N 2 ); IO N LY _C O N T. 1 -O N , 0 -O FF 1 1 ! O U T: 1 -O P T.D E P TH , 2 -A B S ., 3 -TR A N S .; IO P T_M L : 1 -M U LTILA Y E R O P T.D E P TH O U T 1 ! IN TE R P O LA TIO N : 1 -L IN E A R ; 2 -K V A D R A T. 3 ! R E A D L IN E S : 3 -H ITR A N -2004 ; 2 -H ITR A N 96 ; 1 -H ITR A N 91 ; 0 -FR O M LB L_A TL .D A T 0 0 ! ou tpu t: i f 0 - un i fo rm ou t s tep , s e ted abov e (O U T S TE P );

DimerHWHM=30 cm-1; Keq=Curtiss

Ierror/IMTCKD

cm-1

Up, Down & Net radiance at 7km, mW/(m2cm-1srad)

Hit&CKD (Down) Hit&CKD (Up) Hit&CKD (NET) MTCKD contrib. (NET)

100 150 200 250

0

1

2signal=signal*(1+0.05)+10-4 W/(m2cm-1srad)

SZA=45o; Water_column=2.99 g/cm2

dFerr / MTCKDcontr


Recommended