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Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity Fluxes during IHOP Christoph Kiemle, G. Ehret, A. Fix, H. Flentje, G. Poberaj, M. Wirth (DLR) R. M. Hardesty, W. A. Brewer, S. P. Sandberg (NOAA) 6. ISTP, Leipzig, 17.9.2003 Overview • Differential-Absorption-Lidar (DIAL) in the DLR Falcon aircraft • High resolution water vapour measurements of the boundary layer • Co-located wind lidar measurements and vertical humidity fluxes

Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

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Page 1: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

Institut für

Physik der Atmosphäre

High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity Fluxes during IHOP

Christoph Kiemle, G. Ehret, A. Fix, H. Flentje, G. Poberaj, M. Wirth (DLR)R. M. Hardesty, W. A. Brewer, S. P. Sandberg (NOAA)

6. ISTP, Leipzig, 17.9.2003

Overview

• Differential-Absorption-Lidar (DIAL) in the DLR Falcon aircraft• High resolution water vapour measurements of the boundary layer• Co-located wind lidar measurements and vertical humidity fluxes

Page 2: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

IHOP Objectives and DIAL Performance

IHOP 2002missions

Objectives Falconflights

H2Odata

(hh:mm)

aerosoldata

(hh:mm)

H2O /aerosol

in %

BLheterogeneity

11 10:21 25:57 39,9

BL evolution

Improve understanding of the relationshipbetween atmospheric water vapor,surface fluxes and boundary layer

processes as they relate to quantitativeforecasts of precipitation

2 2:29 5:09 48,1

ConvectionInitiation

3 3:19 9:32 34,8

Low level jet

understand and predict the processesthat determine where and when

convection forms5 4:34 10:43 42,7

TOTAL 21 20:43 51:21 40,4

Page 3: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

H2O DIAL: Operators’ seat

with quick-look displayH2O DIAL: Telescope, detectorsand passive cooling unit

On board the DLR Falcon

Page 4: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

DIAL System Parameters and Set-up

Wavelength(nm)

927 1064 532

Pulseenergy (mJ)

12 50 40

Repetitionrate (Hz)

50(on/off)

100 100

Pulselength (ns)

7 15 11

Bandwidth(GHz)

0.14 / 90 0.05 0.05

Detector Si:APD Si:APD(s&p pol)

PMT(s&p pol)

FilterFWHM (nm)

1 1 1

Filter trans.(%)

65 40 55

Telescope Cassegrain, Ø35 cmfield-of-view: 1 - 2 mrad

Dataacquisition

14 bit, 10 MHz

Page 5: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

T,P,q

u,v,w,TAS

Dropsondes:u,v, P,T,q

HRDL:Horizontal & vertical wind speed

DIAL:H2O, AerosolsW'u,v

Falcon payload during IHOP_2002

Page 6: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

H2O DIAL Comparisons with Dropsondes

1

2

3

4

5

6 8 10 12 14

100.21W, 36.56N

June 9, 2002, 12:51 UT

H2O DIAL

Dropsonde

H2O Mixing Ratio [g/kg]

Alt

itu

de

[km

]

1

2

3

4

5

2 4 6 8 10 12 14

102.71W, 36.55N

June 9, 2002, 13:17 UT

H2O DIAL

Dropsonde

H2O Mixing Ratio [g/kg]

Alt

itu

de

[km

]

Page 7: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

High Resolution Backscatter and Water Vapour Cross Section

H2O data: 73 m hor. res., 100 m vert. res. in near range, 300 m in far range; overall stat. error 7%

Page 8: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

Water Vapour Spectra and Variance Profile

0.0 0.2 0.4 0.6 0.8 1.0 1.2

km asl.

water vapor variance profile (g/kg)

uncorr. stat. err. variance (dashed)

2

3.0

2.5

2.0

energy spectra of horizontal water vapor series at 2450m asl.

0.0001

0.001

0.01

0.1

(g/kg)2

10000 1000wavelength [m ]

energy spectra of horizontal water vapor series at 1820m asl.

0.0001

0.001

0.01

0.1

(g/kg)2

10000 1000wavelength [m]

Page 9: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

Method for Estimating the Statistical (Random) Error

autocovariance of horizontal water vapor series at 1820m asl.

-0.2

0.0

0.2

0.4

0.6

(g/kg)2

-2000 -1000 0 1000 2000 3000 4000lag [m]

1.0

1.5

2.0

2.5

3.0

3.5

0 10 20 30

Mean of 450 profiles with zeff = 100 m, x = 146 m (Reference = High resolutions)

Mean of 450 profiles with zeff = 150 m, x = 146 m (Low vertical resolution)

Mean of 225 profiles with zeff

= 100 m, x = 292 m (Low horizontal resolution)

IHOP, 7 June 2002, 17:39 - 17:46:30 UTC

Rel. Stat. Uncert. of Water vapor Mixing Ratio (RMS), %H

eig

ht a

.s.l.

, km

2321 zxq

q

σ2q,instr.

σ2q, atmos.

qq

qerrorRMS noise

Assumption: hor. homogeneity DIAL resolution scaling law

Page 10: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

High Resolution Water Vapor and Vertical Wind

-101.92 -101.90 -101.88 -101.86 -101.84 -101.82lo ng itud e

1.01.5

2.0

2.5

3.0

heig

ht (k

m)

1 .01.5

2.0

2.5

3.0

3.0 3.5 4.0 4.5 5.0 5.5 6.0 6.5 7.0 7.5 8.0 8.5 9.0 9.5 10.0 g /kg

DLR DIAL wa te r va p o ur m ixing ra tio

0 2 4 6 8 10d ista nc e (km )

1.5

2.0

2.5

3.0

3.5

heig

ht (k

m)

1 .5

2.0

2.5

3.0

3.5

-3.5 -3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 m /s

NO AA HRDL ve rtic a l wind ve lo c ity

DLR-DIAL:

x = 150 m

y = 150 m

NOAA-HRDL:

x = 150 m

y = 150 m

Page 11: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

Co-located Airborne Water Vapour and Wind Lidars

Page 12: Institut für Physik der Atmosphäre Institut für Physik der Atmosphäre High Resolution Airborne DIAL Measurements of Water Vapour and Vertical Humidity

Institut für

Physik der Atmosphäre

Estimation of Latent Heat Flux Profile by Eddy Correlation

Flux F = w’q’ q’ = q - q

statistical error (solid):

σ2F, instr. = Δt/T σ2

w atm. σ2q, instr.

Ritter et al., JGR, 1990

sampling error (dashed):

σ2F, sampling =

2 ISF/T (F2 + σ2w atm. σ2

q, atm.)

Lenschow and Stankov, JAS, 1986