ch5: radiative properties of natural surfaces

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Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH5: Radiative Properties of Natural Surfaces BRDF: One of the most general means to characterize the reflection properties of a surface is by use of the bi-directional reflection distribution function (BRDF), a function which defines the spectral and spatial reflection characteristic of a surface. The BRDF of a surface is the ratio of reflected radiance to incident irradiance at a particular wavelength: L = reflected radiance (radiant intensity) and E is the incident irradiance (flux). From http://math.nist.gov/~FHunt/appearance/brdf.html

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Page 1: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

CH5: Radiative Properties of Natural Surfaces

BRDF: One of the most general means to characterize the reflection properties of a surface is by use of the bi-directional reflection distribution function (BRDF), a function which defines the spectral and spatial reflection characteristic of a surface. The BRDF of a surface is the ratio of reflected radiance to incident irradiance at a particular wavelength: L = reflected radiance (radiant intensity) and E is the incident irradiance (flux). From http://math.nist.gov/~FHunt/appearance/brdf.html

Page 2: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Polarization States: A reminder

Wave/Photon boson: Polarization.

Linear Polarization: E-field in one direction.

Circular, elliptical polarization: E-Efield rotates due to phase difference between horizontal and vertical components.From: http://hyperphysics.phy-astr.gsu.edu/hbase/phyopt/polclas.html

Page 3: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

More Details on the Polarization States

Circular Polarization

Elliptical Polarization:

The most general representation.

Page 4: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Fresnel Reflection Coefficients: What is the magnitude of the light specularly reflected from an ice surface as a function of wavelength?

Medium 2

Medium 1

i

t

Page 5: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Here assume n1=n1r, n1i=0, n2=n2r, n2i=0.

MIRAGES

n1sin(1)= n2sin(2)

For a gas, (nr-1) ≈ =gas density.

d/dz > 0 for this type or mirage.

What does this say about the likelihood of convection?

z

Another type of reflection without a real interface.

Mirages can complicate the BRDF

Page 6: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Solar Wavelengths: Reflection + Absorption = Total Radiation

Incident = 1

Reflection = r()

Transmission = Absorption = a()

1 = a() + r()

Page 7: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Radiant Intensity and Flux: How do we deal with reflected radiation?

What are examples of each type of reflection?

Page 8: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Reflection is Complex !!!

Page 9: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Reflection Coefficient of Various Surfaces

Notes: 1. Snow varies greatly with wavelength, especially in the IR.2. Note the straw versus alfalfa (dry dead plant versus live plant).

Page 10: CH5:  Radiative Properties of Natural Surfaces

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

General Case: BDRF BRDF, Bidirectional Reflection Function.

Special Case: Lambertian Surface.

General Case: Why the cos and sin?

General Case: reflectivity