improved orbiting carbon observatory-2 (oco-2) retrievals...

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Page 1 1 of 18 © 2017 California Institute of Technology. Government Sponsorship Acknowledged.

Vijay Natraj (Jet Propulsion Laboratory, California Institute of Technology)

Co-Authors Matthäus Kiel (Caltech)

Aronne Merrelli (University of Wisconsin-Madison/SSEC) James McDuffie (JPL/Caltech) Brendan Fisher (JPL/Caltech)

Chris O’Dell (Colorado State University) David Crisp (JPL/Caltech)

Annmarie Eldering (JPL/Caltech) Dejian Fu (JPL/Caltech)

Debra Wunch (University of Toronto) Paul Wennberg (Caltech)

Lukas Mandrake (JPL/Caltech)

13th International Workshop on Greenhouse Gas Measurements from Space June 6, 2017

Improved Orbiting Carbon Observatory-2 (OCO-2) Retrievals Using a BRDF Model for the

Surface

Page 2 2 of 18

Retrieved Albedo Correlated With Scattering Angle

Retrieved albedo correlated with scattering angle => BRDF effects?

Page 3 3 of 18

OCO-2 Measurement Geometry

Page 4 4 of 18

•  w: overall BRDF amplitude [BRDF weight] •  s: slope of BRDF amplitude [BRDF weight slope] •  λ: wavelength •  λ0: reference wavelength (where parameters are retrieved) •  F: function describing BRDF shape (RPV kernel) •  ρ0: hot spot parameter = 0.05 •  θ: asymmetry parameter = −0.1 •  k: anisotropy parameter = 0.75 •  BRDF kernel reduces to Lambertian kernel for certain choice of BRDF shape

parameters •  w, s retrieved

BRDF Formulation

BRDF(λ) = w+ s(λ −λ0 )[ ]F(ρ0,ϑ ,k)

Page 5 5 of 18

RPV Kernel Shape

Page 6 6 of 18

•  w and s converted to more physically meaningful quantities, ρw (reflectance) and ρs (reflectance slope)

•  ρw and ρs calculated by evaluating the BRDF kernel model at the primary observation geometry

•  Reflectance factor equals ratio between reflected radiance and that from pure Lambertian surface at the same geometry

•  For no scattering scenario, this is equivalent to a Lambertian albedo

•  Consistency between Lambertian albedo used in B7 and effective albedo used in B8

BRDF Outputs

Page 7 7 of 18

Number of Converged Soundings

Page 8 8 of 18

Retrieved AOD (Bremen, 9090)

Page 9 9 of 18

Retrieved AOD (Caltech, 3052)

Page 10 10 of 18

Retrieved XCO2 (Bremen, 9090)

Page 11 11 of 18

Retrieved XCO2 (Caltech, 3052)

Page 12 12 of 18

Retrieved Albedo (Bremen, 9090)

Page 13 13 of 18

Retrieved Albedo (Caltech, 3052)

Page 14 14 of 18

Retrieved BRDF Weights (Bremen, 9090)

Page 15 15 of 18

Retrieved BRDF Weights (Caltech, 3052)

Page 16 16 of 18

•  To-do items from last year implemented ü  Re-baseline with new spectroscopic models ü  How do we compare Lambertian and BRDF results ü  Implement BRDF model in operational code

•  Increased convergence

•  Improved AOD retrievals

•  Reduced scatter in XCO2 retrievals

•  Consistency in albedo values between B7 and B8

•  Strong correlation of albedo with scattering angle

•  Little correlation between BRDF weight and scattering angle

Conclusions

Page 17 17 of 18

Backup Slides

Page 18 18 of 18

OCO-2 Science Viewing Modes

Nadir Observations: + Small footprint (< 3 km2) - Low Signal/Noise over dark

surfaces (ocean, ice)

Glint Observations: + Improves Signal/Noise over

oceans - More cloud interference

Target Observations: •  Validation over ground

based FTS sites, field campaigns, other targets

447-

m W

LEF

Tow

er

Park Falls, WI Local Nadir

Glint Spot

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