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Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium.

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Page 1: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

CH4: Reflection and Refraction in a Homogenous Medium.

Page 2: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

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: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

More Details on the Polarization States

Circular Polarization

Elliptical Polarization:

The most general representation.

Page 4: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Three Choices for Solar Radiation

Emissivity is the same as absorptivity. Source can be visible or infrared radiation, or other wavelengths as well, microwave, etc.

Transmission + Reflection + Absorption = 1

Page 5: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Reflection, Refraction, and Transmission

Page 6: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

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 7: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Trace velocity matching principle: Snell’s law (continuity of the wavefront at a boundary)

“slow is more normal”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.

Page 8: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Snell’s Law: Kinematics

Page 9: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Complex Refractive Index for Water and Ice

Page 10: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Some Basics, Electromagnetic Skin Depth

Page 11: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Wave Penetration Depth in Water and Ice

Page 12: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Boundary Conditions at Interfaces: Used with Plane Wave Solutions of Maxwell’s Equations for E and H to get the Fresnel Coefficients.

• Used along with boundary conditions to calculate the single scattering properties of aerosols and hydrometeors (cloud droplets, rain drops, ice crystals, snow flakes, etc), from first principles if possible. {Mie theory for homogeneous spheres, coupled dipole theory for general particles, T-Matrix method, etc}

• Are not used to calculate the radiation field arriving at the surface from the complex atmosphere. Multiple scattering theory is used.

Page 13: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Fresnel Reflection Coefficients: What is the magnitude of the light specularly reflected from a surface? (Also can get the transmitted wave magnitude).

Medium 2

Medium 1

i

t

Page 14: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Reflectivity of Water And Ice

BrewsterAngle

Microwave =15,000 microns nr = 6.867192 ni = 2.630

Mid Visible (green) =0.5 microns nr = 1.339430 ni = 9.243 x 10-10

Page 15: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Reflectivity of Water And Ice: Normal Incidence

What drives the reflectivity?

Page 16: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Geometrical Optics: Interpret Most Atmospheric Optics from Raindrops and lawn sprinklers (from Wallace and Hobbs CH4)

Rainbow from

raindrops

Primary Rainbow Angle: Angle of Minimum Deviation (turning point) for rays incident with 2 chords in raindrops.

Secondary Rainbow Angle: Angle of Minimum Deviation (turning point) for rays incident with 3 chords in raindrops.

Page 17: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Rainbow Optics

scattering angle

See http://www.philiplaven.com/p8e.html, and atmospheric optics.

nr

Page 18: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Geometrical Optics: Rainbow (from Petty)

Angle of minimum deviation from the forward direction. Focusing or confluence of rays.

x

Distance x is also known as the impact parameter. (Height above the sphere center.)

Page 19: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Geometrical Optics: Interpret Most Atmospheric Optics from Ice Crystals (from Wallace and Hobbs CH4)

22 deg and 45 deg Halos from cirrus crystals of the column or rosette (combinations of columns) types. Both are angle of deviation phenomena like the rainbow. Crystal orientation important. 22 deg halo, more common, thumb rule to measure size of arc.

Page 20: Pat Arnott, ATMS 749 Atmospheric Radiation Transfer CH4: Reflection and Refraction in a Homogenous Medium

Pat Arnott, ATMS 749 Atmospheric Radiation Transfer

Light Scattering Basics (images from Wallace and Hobbs CH4).

Sphere, radius r, complex refractive index n=mr + imi

x

xxLines :

r= x2π

Dimensionless Parameters

SizeParameter≡x=2πr

ScatteringEfficiency≡Qs=σscaπr2

mr=1.5

Qs

Angular Distribution of scattered radiation (phase function)

x x

xDipole scattering