objective theory some initial results - asr...norm. zen.rad. (red) cod(red) cod(red) clou dop tica...

1
Stephen E. Schwartz and Dong Huang Brookhaven National Laboratory, Upton NY [email protected] [email protected] http://www.ecd.bnl.gov/steve Daniela Viviana Vladutescu New York City College of Technology, CUNY [email protected] Short-Range Structure of Cloud Optical Depth in North Central Oklahoma Determined by High Resolution Photography From the Surface Atmospheric Systems Research Science Team Meeting, May 2-5, 2016 RADIATION TRANSFER CALCULATIONS WITH DISORT NORMALIZED ZENITH RADIANCE: Zenith radiance per incoming direct normal solar irradiance, function of cloud optical depth (COD) and solar zenith angle (SZA) W m -2 nm -1 sr -1 per W m -2 nm -1 , or sr -1 Rayleigh sky is dark. Clouds initially increase zenith radiance . 4 6 0.01 2 4 6 0.1 2 4 6 1 r s , e c n a i d a r d e z i l a m r o N -1 0.001 0.01 0.1 1 10 100 Cloud optical depth cos (SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 Solid, 460 nm Dashed, 640 nm 0.25 0.20 0.15 0.10 0.05 0.00 Norm. radiance, sr-1 10 8 6 4 2 0 Cloud optical depth Red Blue CLOUD ALBEDO calculated from COD Cloud albedo is nearly independent of color. Cloud albedo varies linearly with COD for COD 3. < ~ 2 4 6 8 0.1 2 4 6 8 1 Albedo 0.01 0.1 1 10 100 Cloud optical depth cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 Blue Red 10 -5 10 -4 10 -3 10 -2 10 -1 10 0 Cloud albedo 0.01 0.1 1 10 100 Cloud optical depth cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 Blue Red Slope = 1 Red/(Red + Blue) a commonly used cloud discriminant: Define RADIATIVE CLOUD FRACTION, a variable that ranges from 0 to 1 as COD increases: Radiative cloud fraction can be determined on pixel-by-pixel basis. COLOR: Sky is blue, clouds are white r RRB (μ 0 , ) = R R nz (μ 0 , ) R R nz (μ 0 , ) + R B nz (μ 0 , ) 0.6 0.5 0.4 0.3 0.2 0.1 0.0 Red/(Red + Blue) 10 8 6 4 2 0 Cloud optical depth cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 0.30 F r (μ 0 , ) r RRB (μ 0 , ) r RRB (μ 0 ,0) 3 1.2 1.0 0.8 0.6 0.4 0.2 0.0 Radiative cloud fraction 10 8 6 4 2 0 Cloud optical depth cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 0.30 For Red = 640 nm and Blue = 460 nm, Red/(Red + Blue) ranges from about 0.22 to 0.52 with increasing COD. CLOUD OPTICAL DEPTH by inverting radiance 0.2 0.1 0.0 0.05 0.00 6 5 4 3 2 1 0 Cloud optical depth 0.25 0.20 0.15 0.10 0.05 0.00 Normalized zenith radiance, sr -1 640 nm, Red 460 nm, Blue Cos (SZA) = 0.85 0.25 0.20 0.15 0.10 0.05 0.00 Normalized zenith radiance, blue, sr -1 0.25 0.20 0.15 0.10 0.05 0.00 Normalized zenith radiance, red, sr -1 Descending, High COD Ascending, Low COD 1:1 line COD is not monotonic; inversion is limited to thin clouds, COD < ~ 3. APPROACH Characterize cloud radiative properties at high resolution from the surface. Digital photography with long-focal-length lens. Camera facing upwards takes photos at regular intervals. Use radiative transfer model to relate counts in camera to radiance and then to cloud optical depth, cloud albedo, radiative cloud fraction. COMMERCIALLY AVAILABLE HIGH-RESOLUTION CAMERA 1200 mm equivalent 35 mm focal length; f / 5.6 vs. $350 Todd Vorenkamp, B&H Photo, NYC $180,000 Nominal resolution 6 μrad (6 mm at 1 km) a b c d e f 1680 1660 1640 1620 1600 1580 1560 2280 2240 2200 2160 1900 1800 1700 1600 1500 1400 1300 2500 2300 2100 1900 3000 2500 2000 1500 1000 500 0 4000 3000 2000 1000 0 2 cm 4 cm 8 cm 1 cm 1625 1620 1615 1610 1605 1600 2250 2240 2230 2220 2210 2200 65x10 3 60 55 50 Counts 2250 2240 2230 2220 2210 2200 RESOLVING POWER TEST AT 1 km Actual resolution 20 μrad (20 mm at 1 km) 17 34 69 86 0.3 0.6 0.9 1.2 1.5 1.8 103 radians East West North South 12:00 16:00 14:00 18:00 20:00 22:00 24:00 degrees 52 Sun, angular diameter 0.535˚ = 9.3 mrad Narrow FOV Camera, 22 x 29 mrad = 2 x 3 sun diameters Both drawn 10 times actual angular dimension Wide FOV Camera, 120 x 160 mrad, Actual angular dimension Moonshot for comparison Time is UTC; local sun time = UTC - 6.5 h. OBSERVATION GEOMETRY 10x10 3 8 6 4 2 0 Sensitivity , counts J -1 , relative 900 800 700 600 500 400 300 Wavelength, nm WAVELENGTH CALIBRATION Integrating sphere, Hg-Xe lamp, Calibrated photodiode Peaks: 460, 640 nm Identify darkest and brightest regions of images to determine C min and C max . Scaled normalized radiance R s is evaluated from measured counts C as R s = R min + C C min C max C min ( R max R min ) R min and R min are from radiation transfer calculations. Agreement of scaled radiances with theory lends confidence to the approach. SCALING OF RADIANCES from images ZOOMING IN, IN SPACE AND TIME FIVE MINUTES IN OKLAHOMA 07-31-2015; UTC time; local sun time = UTC - 6.5 h; 16:34 = 10:04 sun time. Wide field of view 240 × 320 m Narrow field of view 43 × 57 m CLOUD OPTICAL DEPTH by inverting radiance RGB Red Red COD(Red) COD(Blue) COD(Blue) vs COD(Red) COD(Blue) vs COD(Red) Image 1028 Image 1028 Image 1041 COD(Red) COD(Blue) RGB Red Red Image 1041 Acknowledgments Supported by the U.S. Department of Energy (DOE) Atmospheric System Research Program (Office of Science, OBER) under Contract No. DE-AC02-98CH10886. We thank the staff at the ARM Central Great Plains site in Lamont, OK, particularly Matt Gibson and James Martin, for assistance in the deployment. Pilot studies at Brookhaven National Laboratory were carried out with Antonio Aguirre (New York City College of Technology, Brooklyn), with support from the National Science Foundation, Louis Stokes Alliance for Minority Participation (LSAMP), and Clement Li (City College of the City University of New York) with support from the DOE Office of Science, Office of Workforce Development for Teachers and Scientists under the Visiting Faculty Program. CONCLUSIONS Photography of clouds from the surface provides a novel way of looking at clouds and their radiative effects at much higher resolution than other cloud imaging techniques. Readily available commercial cameras provide a resolution of about 20 μrad (corresponding to 4 cm for cloud base at 2 km), 3 orders of magnitude higher than typical satellite products. Cloud properties are highly variable in space (a few meters or less) and time (a few seconds or less). Manuscript about to be submitted! Cloud optical depth can be accurately retrieved at native resolution of the camera for optically thin clouds, optical depth < 3. ~ 10 Million determinations of COD, cloud albedo, radiative cloud fraction, etc.,for each image. Images and analyses of these should be of value to cloud modelers. Doppler Lidar: Thin wimpy clouds Image 1028 Image 1041 Cloud albedo (Red) Cloud albedo (Blue) Radiative Cloud Fraction CLOUD ALBEDO and CLOUD RADIATIVE FRACTION PDF 0.12 0.08 0.04 0.00 Cloud albedo Image1028 Image1041 PDF 1.0 0.8 0.6 0.4 Radiative cloud fraction Image1028 Image1041 RGB Image 1041 Norm. Zen.Rad. (Red) COD(Red) Norm. Zen.Rad. (Red) COD(Red) COD(Red) Cloud optical depth structure at CENTIMETER SCALES THEORY OBJECTIVE SOME INITIAL RESULTS

Upload: others

Post on 24-Dec-2020

1 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: OBJECTIVE THEORY SOME INITIAL RESULTS - ASR...Norm. Zen.Rad. (Red) COD(Red) COD(Red) Clou dop tica ep h structure at EN TIM R SCAL OBJECTIVE THEORY SOME INITIAL RESULTS Title agu poster

Stephen E. Schwartz and Dong HuangBrookhaven National Laboratory, Upton NY

[email protected] [email protected]://www.ecd.bnl.gov/steve

Daniela Viviana VladutescuNew York City College of Technology, CUNY

[email protected]

Short-Range Structure of Cloud Optical Depth in North Central Oklahoma Determined by High Resolution Photography From the Surface

Atmospheric Systems Research Science Team Meeting, May 2-5, 2016

RADIATION TRANSFER CALCULATIONS WITH DISORT

NORMALIZED ZENITH RADIANCE: Zenith radiance per incoming direct normal solar irradiance, function of cloud optical depth (COD) and solar zenith angle (SZA)

W m-2 nm-1 sr-1 per W m-2 nm-1, or sr-1

Rayleigh sky is dark. Clouds initially increase zenith radiance.

46

0.012

46

0.12

46

1rs ,ecnaidar dezilamro

N-1

0.001 0.01 0.1 1 10 100Cloud optical depth

cos (SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50

Solid, 460 nmDashed, 640 nm

0.25

0.20

0.15

0.10

0.05

0.00Nor

m. r

adia

nce,

sr-1

1086420Cloud optical depth

Red Blue

CLOUD ALBEDO calculated from COD

Cloud albedo is nearly independent of color.Cloud albedo varies linearly with COD for COD 3.<~

2

4

68

0.1

2

4

68

1

Albe

do

0.01 0.1 1 10 100Cloud optical depth

cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50

BlueRed

10-5

10-4

10-3

10-2

10-1

100

Clo

ud a

lbed

o

0.01 0.1 1 10 100Cloud optical depth

cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50

BlueRed

Slope = 1

Red/(Red + Blue) a commonly used cloud discriminant:

Define RADIATIVE CLOUD FRACTION, a variable that ranges from 0 to 1 as COD increases:

Radiative cloud fraction can be determined on pixel-by-pixel basis.

COLOR: Sky is blue, clouds are white

rRRB(μ0, )= RRnz(μ0, )

RRnz(μ0, )+ RB

nz(μ0, )

0.60.50.40.30.20.10.0R

ed/(R

ed +

Blu

e)

1086420Cloud optical depth

cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 0.30

Fr (μ0, ) rRRB(μ0, ) rRRB(μ0,0)3

1.21.00.80.60.40.20.0

Rad

iativ

e cl

oud

fract

ion

1086420Cloud optical depth

cos(SZA) 1.00 0.95 0.90 0.85 0.80 0.70 0.60 0.50 0.30

For Red = 640 nm and Blue = 460 nm, Red/(Red + Blue)ranges from about 0.22 to 0.52 with increasing COD.

CLOUD OPTICAL DEPTH by inverting radiance

0.2

0.1

0.00.050.00

6543210C

loud

opt

ical

dep

th

0.250.200.150.100.050.00Normalized zenith radiance, sr-1

640 nm, Red 460 nm, Blue

Cos (SZA) = 0.850.25

0.20

0.15

0.10

0.05

0.00Nor

mal

ized

zen

ith ra

dian

ce, b

lue,

sr-1

0.250.200.150.100.050.00

Normalized zenith radiance, red, sr-1

Descending,High COD

Ascending,Low COD

1:1 line

COD is not monotonic; inversion is limited to thin clouds, COD <~ 3.

APPROACHCharacterize cloud radiative properties at high resolution

from the surface.

Digital photography with long-focal-length lens.Camera facing upwards takes photos at regular intervals.Use radiative transfer model to relate counts in camera to

radiance and then to cloud optical depth, cloud albedo,radiative cloud fraction.

COMMERCIALLY AVAILABLEHIGH-RESOLUTION CAMERA

1200 mm equivalent 35 mm focal length; f / 5.6

vs.

$350Todd Vorenkamp, B&H Photo, NYC

$180,000Nominal resolution 6 µrad (6 mm at 1 km)

a

b

c

d

e

f

1680

1660

1640

1620

1600

1580

1560

2280224022002160

1900

1800

1700

1600

1500

1400

1300

2500230021001900

3000

2500

2000

1500

1000

500

0

40003000200010000

2 cm

4 cm

8 cm

1 cm

1625

1620

1615

1610

1605

1600

225022402230222022102200

65x103

60

55

50Cou

nts

225022402230222022102200

RESOLVING POWER TEST AT 1 km

Actual resolution 20 µrad (20 mm at 1 km)

17 34 69 86

0.3

0.6

0.9

1.2

1.5

1.8

103

radians

East West

North

South

12:00

16:00

14:00

18:00 20:0022:00

24:00

degrees52

Sun, angular diameter 0.535˚ = 9.3 mrad

Narrow FOV Camera, 22 x 29 mrad = 2 x 3 sun diameters

Both drawn 10 times actual angular dimension

Wide FOV Camera, 120 x 160 mrad,Actual angular dimension

Moonshotfor comparison

Time is UTC; local sun time = UTC - 6.5 h.

OBSERVATION GEOMETRY

10x103

8

6

4

2

0Sens

itivi

ty, c

ount

s J-1

, rel

ativ

e

900800700600500400300Wavelength, nm

WAVELENGTHCALIBRATIONIntegrating sphere,Hg-Xe lamp,Calibrated photodiodePeaks: 460, 640 nm

Identify darkest and brightest regions of images to determine Cmin and Cmax. Scaled normalized radiance Rs is evaluated from measured counts C as

Rs = Rmin +C Cmin

Cmax Cmin(Rmax Rmin )

Rmin and Rmin are from radiation transfer calculations.Agreement of scaled radiances with theory lends confidence to the approach.

SCALING OF RADIANCES from images

ZOOMING IN, IN SPACE AND TIMEFIVE MINUTES IN OKLAHOMA

07-31-2015; UTC time; local sun time = UTC - 6.5 h; 16:34 = 10:04 sun time.Wide field of view 240 × 320 m

Narrow field of view 43 × 57 m

CLOUD OPTICAL DEPTH by inverting radianceRGB Red Red

COD(Red) COD(Blue) COD(Blue) vs COD(Red)

COD(Blue) vs COD(Red)

Image1028

Image1028

Image1041

COD(Red) COD(Blue)

RGB Red Red

Image1041

AcknowledgmentsSupported by the U.S. Department of Energy (DOE) Atmospheric System Research Program (Office of Science, OBER) under Contract No. DE-AC02-98CH10886. We thank the staff at the ARM Central Great Plains site in Lamont, OK, particularly Matt Gibson and James Martin, for assistance in the deployment. Pilot studies atBrookhaven National Laboratory were carried out with Antonio Aguirre (New York City College of Technology, Brooklyn), with support from the National Science Foundation, Louis Stokes Alliance for Minority Participation (LSAMP), and Clement Li (City College of the City University of New York) with support from the DOE Office of Science, Office of Workforce Development for Teachers and Scientists under the Visiting Faculty Program.

CONCLUSIONSPhotography of clouds from the surface provides a novel way of looking at clouds and their radiative effects at much higher resolution than other cloud imaging techniques.

Readily available commercial cameras provide a resolution of about 20 µrad (corresponding to 4 cm for cloud base at 2 km), 3 orders of magnitude higher than typical satellite products.

Cloud properties are highly variable in space (a few meters or less) and time (a few seconds or less).•

Manuscript about to be submitted! •

Cloud optical depth can be accurately retrieved at native resolution of the camera for optically thin clouds, optical depth < 3.~

10 Million determinations of COD, cloud albedo, radiativecloud fraction, etc.,for each image.

•Images and analyses of these should be of value to •cloud modelers.

Doppler Lidar: Thin wimpy clouds

Image1028

Image1041

Cloud albedo (Red) Cloud albedo (Blue) Radiative Cloud FractionCLOUD ALBEDO and CLOUD RADIATIVE FRACTION

PDF

0.120.080.040.00Cloud albedo

Image1028 Image1041

PDF

1.00.80.60.4Radiative cloud fraction

Image1028 Image1041

RGB Image 1041 Norm. Zen.Rad. (Red) COD(Red)

Norm. Zen.Rad. (Red) COD(Red)COD(Red)

Cloud optical depth structure at CENTIMETER SCALES

THEORYOBJECTIVE SOME INITIAL RESULTS