Atmospheric Optics Karen J. Meech, Astronomer Institute for Astronomy Lecturer: Jan Kleyna Electromagnetic Radiation ! Characterized by !, f, c ! Speed c = 3x10 5 km/s in vacuum ! Velocity not constant in other media ! Because of charge separation " slowing ! Index of refraction: n = c/v ! Speed decreases for shorter !, hard to get molecule to oscillate ! Results in dispersion Medium n Air 1.0003 Water 1.333 Glass 1.4-1.9 Medium n CO 2 1.00045 Benzene 1.501 Diamond 2.419
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Atmospheric Optics
Karen J. Meech, Astronomer
Institute for Astronomy
Lecturer: Jan Kleyna
Electromagnetic Radiation
! Characterized by !, f, c ! Speed c = 3x105 km/s in vacuum ! Velocity not constant in other media
! Because of charge separation " slowing
! Index of refraction: n = c/v ! Speed decreases for shorter !, hard to
get molecule to oscillate ! Results in dispersion
Medium n Air 1.0003
Water 1.333 Glass 1.4-1.9
Medium n CO2 1.00045
Benzene 1.501 Diamond 2.419
Huygen’s Principle (1678) ! Wave theory for light ! Model for behavior ! Not a physical theory ! Light as a wavefront
! Think of an advancing ‘plane wave’ as a set of point-like emitters (1)
! The spherical waves from the points add up and cancel out to make a new plane wave a moment later (2)
! ... so wave advances
(1) (2)
4
Wave Nature Implies Refraction (bending)
Air (fast, n≅1)Glass (slow, n>1.4)
! Mechanism ! As waves travel from faster
medium (air) to slower (glass) the wave front slows
! If light hits the boundary at an agle, one side of front slows first
! The light bends ! Analogy
! Tires on one side of wagon slow down in mud, and wagon turns toward the mud
At each interface there is both
! Light bent towards the perpendicular nlow " nhigh
! Light bent away from perpendicular nhigh " nlow
"1#
"2#
n1
n2 > n1
n2 < n1 "2#
Refraction Reflection
! ! = Angle of reflection = Angle of incidence
Dispersion
1 2
• How does a prism work? • nair = 1.0003 < nglass ~ 1.5 • 1 - bent toward ⟂ • 2 - bent away from ⟂
• Recall that nglass changes with wavelength
• blue refracts more than red • higher frequency " bent
more " dispersion of white light into spectrum
Applications: Atmospheric Refraction
! Starlight passes from vacuum, n=1.000 into the atmosphere, n=1.0003
! Density of air increases at lower altitudes " n changes ! As n increases, light is bent continuously, deflecting star ! Blue light bent the most
! “Differential refraction” " colorful stars, especially near horizon
8
Green Flash – Atmospheric Refraction
! Differential refraction ! Uppermost part of sun’s disk
is bluer when near horizon
! Sun sets ! Red sets first ! Green / Blue sets last because air is bending it over horizon
! Blue hard to see because of atmospheric scattering ! Sky is blue, which means that atmosphere scatters blue light in all
directions instead of transmitting it ! Thus green is usually the last visible bit of the sun
Green flash really has several types, involving multiple refraction phenomena, including mirages - for more information, see
http://mintaka.sdsu.edu/GF/papers/Zenit/GF.html
Demo Break
! Refraction at different angles ! Scattering vs. Absorption in Atmosphere ! Greenflash ! Interstellar reddening & extinction ! “Seeing”
The Rainbow ! Rene Descartes 1637
! rainbow physics from experiments with glass spheres filled water
! Rainbow is seen ! 42o away from anti-solar
direction
! Each person has a “personal” rainbow
! you see blue at angles where the droplets send just blue light into your eye
From Sun
Rainbow Formation
! Combination of refraction & reflection at each interface ! Light entering perpendicular – passes
through w/o refraction ! Light enters at angle refracted &
reflected at each boundary " light loss ! Dispersion of different ! of light occurs
! Light at back of drop: refracted & reflected ! Light returns to front of drop
! Light farther from central axis " refracted farther until reaching a critical point ! At critical point, rays cross
! Raindrop: water ! n = 1.333
! In Air ! n = 1.0003
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Tracing rays of light in a sphere of water ! Rays from 2"7 emerge
farther from center ! Beyond ray 7, refracted ray
moves toward center ! Light bunches up (gets
brighter at crossover) ! Angle between ray 1 and 7 is
~42o " this is the RAINBOW
! Red refracted least " on outside of rainbow
A rainbow arises from the special geometry of reflection+ refraction in a sphere, plus dispersion
IN
OUT
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Circular Rainbows
! Only visible from certain geometric perspectives " above the ground
! Only visible from certain geometric perspectives " above the ground
You are at the ocean. You see a rainbow in the salt spray. You know that salt water has a slightly larger index of refraciton than fresh water. The salt spray rainbow has an angular diameter that is:
A. Smaller than normal (freshwater) rainbow B. Larger than a normal rainbow
C. The same size as a normal rainbow D. It depends on the angle of the sun
?°Clicker: Discuss in Groups
You are at the ocean. You see a rainbow in the salt spray. You know that salt water has a slightly larger index of refraciton than fresh water. The salt spray rainbow has an angular diameter that is:
A. Smaller than normal (freshwater) rainbow B. Larger than a normal rainbow
C. The same size as a normal rainbow D. It depends on the angle of the sun
?°Clicker: Second chance
20
Answer: A - smaller, because index of refraction is larger, so light is refracted more, so rainbow angle is less than 42°
! Primary: Red on outside ! Red is refracted least
! Secondary: Red on inside ! Internal reflection
! Brighter region inside first bow ! all light that hits droplets is
scattered inside 42° critical angle, so region inside rainbow is bright
Bright Region
23
What happens to rainbow if droplets are not spheres?
A. Droplets have to be very close to spherical. If they aren’t, there’s no rainbow.
B. If droplets aren’t spheres, the rainbow won’t be circular, but will be flattened or elongated.
C. If droplets are circular along some direction (or axis), then some parts of the rainbow will form, leading to a 42° circular (but broken or incomplete) rainbow.
D. Flat droplets lead to a rainbow larger than 42°, and elongated droplets to a rainbow smaller than 42°.
23 Hint - think of a water glass
24
Answer: C
The dimension of a droplet that is circular will lead to a rainbow. The non-circular dimensions won’t lead to a rainbow. So non-circular droplets lead to broken rainbows that still obey the 42° rule.
Raindrop Shape Effects
! Rainbows require a circular cross section
! Raindrops can be large ! gravity distorts shape
! Rainbow seen only at certain orientations ! Corresponds to horizontal circular
cross section
Fogbows & Redbows ! Fogbow
! Very tiny droplets suspended in cloud/mist
! Same physics, colors overlap ! Bow looks white because
wavelength becomes larger compared to drop size - geometrical optics doesn’t quite work and colors blend
! Red Rainbow ! Blue light is more easily
scattered in atmosphere ! Remaining light mostly red,
orange, yellow
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What is Wrong with this Picture?
A. Colors not reversed on 2nd rainbow
B. 3rd bow should not exist
C. Hillside not illuminated
D. Region inside first bow is not bright
E. A,B, C, and D
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Answer: E (all of the above)
What other things are wrong with it?
A. Colors not reversed on 2nd rainbow
B. 3rd bow should not exist
C. Hillside not illuminated
D. Region inside first bow is not bright
E. A,B, C, and D
Alien Rainbows?
! n = 1.333 ! n = 0.749
Atmospheric Structure ! Troposphere cools with
increasing altitude ! T < 273K until ionosphere ! Clouds contain ice crystals
! Displays affected by: ! Different crystal shapes ! Different light paths
through crystals
! Give information on ice in the upper atmosphere
Ice Crystal Refraction - Halos
! Flat (plate) hexagonal crystals: prisms ! Rays deflected through many angles
(22 to 50 deg) depending in incidence angle
! Colors ! Red refracted least " inside ! Blue refracted most " outside
! Orientation ! Minimum angle of deviation 22o
! Random " 22o halo ! Parallel to Earth " horizontal parts
only " “Sundog”
" = 22o
33
Halos: Why do randomly oriented crystals cause a ring?
Many different rotation angles cause a deflection very close to 22°.
Halos & Sundogs (Parhelia)
! Sundogs – most often seen when sun is low
Sun Pillars
! Reflection of light from flat plate crystals ! Intensity & height depends on crystal
orientation ! Pillars can be any color
Sunset Pillar Moon Pillar Venus Pillar
Complex Displays • CZA
• horiz. ice crystals; light enters through top face and exits side face
• UTA • Long, horizontal oriented
cyrstals • Like 22o halo or sundog • Except for crystal orientation
• Parhelic circle • Reflection of light from vertical
ice crystals • Simple, or internal with color
dispersion • LTA
• Long, horizontal crystals, the twin of the UTA
Tangent Arcs & Circumscribed Halos
! Formed by pencil shaped crystals ! Shape of arc depends on sun’s elevation ! Special crystal orientations occur for a narrow
range of sizes: 0.05 – 2 mm; otherwise random
40
22° halos exist because
A. Hexagonal ice crystals align in the sky to focus sunlight at the observer like a lens
B. Hexagonal ice crystals populate the sky at all possible random orientations, but lots of these random orientations refract incoming light at close to 22°
C. Hexagonal ice crystals block light coming directly from the sun, but reflect light from the sides at 22°
D. A 22° halo is the third rainbow, between the sun and the observer
E. None of the above
41
Answer: B
Hexagonal ice crystals populate the sky at all possible random orientations, but lots of these random orientations refract incoming light at close to 22°
If you rotate a hexagonal ice crystal while shining light through it, the outgoing light will be refracted at 22° for a disproportionately large part of the rotation. So if you observe at a random cloud of hexagonal ice crystals, a disproportionate number will be refracting incoming light at 22°. picture here
Parry Arcs (rare:first seen during 1820 arctic expedition)
! Appearance similar to tangent arcs ! crystal horizontal and top/bottom
faces are horizontal ! how this happens still under study
(2010) ! Clusters of pencil crystals? ! Distorted/flattened crystals?
Altitude of Sun
Complex Parry Display
Lowitz Arcs
! More rare than Parry arcs ! Horizontally aligned plate crystals spin
horizontally? ! Origin now in question. ! 3 ray paths give 3 different arcs (upper, lower,
middle)
Middle
Upper
Lower
Lowitz Arc Display
More Complex Displays
Atmospheric Archaeology
! Computer simulations can untangle the optics
! This gives knowledge about ice crystals in Earth’s atmosphere 100’s of years past!
! There are many records of atmospheric light displays
! Simulation ! Pencil crystals, long axes horizontal ! Reflection from end faces of pencils ! Plate crystals for sun dogs
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Review
! Rainbows are caused by ! refraction, reflection, and dispersion
inside water droplets.
! Complex displays ! Sunlight reflecting and refracting in
hexagonal crystals of ice high up in atmosphere can cause complex patterns in the sky, depending on ! light path in crystal ! alignment of crystals in the sky
Randomly oriented ice crystals (halo)
Flat hexagonal plates
Horizontally aligned ice crystals
Parry aligned ice crystals (horizontal and flat face on top)
All of them together recreate Parry Arctic Expedition display of 1820
Demo Break
! Halo Sim Software ! free - runs on Windows (or
Mac with PlayOnMac)
! www.atoptics.co.uk
! St. Petersburg Display of 1790
Compare computation to Lowitz drawing from 1790
Doesn’t look exactly identical: different sky-map projections, like different camera lenses
Supernumerary Bows
! Like the 42° droplet path, but cannot be explained by Geometric optics
! Interference between optical paths close together in water drops (like an oil slick)
! Seen only when drops are very small and of same size - a first proof (1803) that light was made of waves
[*] image from http://www.itp.uni-hannover.de/~zawischa/ITP/refraction.html
*
Optical Effects in Mists ! Water in clouds, mists, fog
! 10-1000x smaller than raindrops ! Wave properties of light
important ! Diffraction Features
! Corona – rings around the sun ! Glory – ringed phenomena opposite
the sun ! Spectre de Brocken ! Iridescent Clouds ! Heligenschein
Interference – Light superposition
! Light is a wave ! Amplitude of wave related
to intensity (or brightness)
! Combining EM radiation ! add amplitude of wave ! In phase: n!, double ! Out of phase n!/2 " 0
Diffraction ! Passing light through a slit ! Use Huygen’s model ! Each point along slit " new waves ! If pathlength in phase " constructive:
a sin " = n!#! Pathlength out of phase " destructive:
a sin " = n!/2 ! Rules of thumb
! " is larger for large ! " red outside ! " is larger for small a " big rings =
small drops ! Any obstacle works " water drops
in cloud
Demo – single slit diffraction
Coronae ! Visible as a ring of colors around the sun or moon
! Ring is close to light source (few degrees) a sin" = n !/2
first dark ring, n = 1; solve for a a = !/2 / sin" 6500/2 / sin (5) = 3.7x104 A a = 3.7 microns
! Particles must be small! ! Any substance ok: water, ice,
dust, pollen
! Multiple sizes " white ring ! More commonly seen around
! Multiple sizes " colored rings overlap " white ! Particles get large " less diffraction, smaller
rings
Glory, Specter de Brocken ! Glory
! Diffraction effect – anti-solar direction (still debated)
! Specter de Brocken ! Seen on Brocken
mountain in Germany ! Glory + 2D or 3D shadow
Cloud Irridescence
! Diffraction effect ! maps out changing cloud
particle sizes
! Nacreous clouds ! Polar stratospheric clouds 25
km high ! High winds ! 10 µm ice crystals ! Often brighter, long lasting
Heiligenschein
! Dew drops on tips of grass ! Large drops " Geometric
optics, not diffraction ! Focus sunlight ! Light scattered back through
drop in direction of sunlight ! A bit like a bicycle reflector
The Opposition Effect
! Opposition Effect ! Enhanced backscattering ! Shadow covering ! Any particulate surface
Other Gases?
! Carbon Dioxide ice ! cubic, octahedral, and cubo-octahedral
Alien Displays – Mars ! Mars Atmosphere
! 95% CO2
! P = 0.006 bar ! Index of refraction
gaseous CO2: 1.00045
! Simulation ! 22o halo – water ice ! Cuboctahedral CO2 ice "
26o halo ! Cuboctahedral plates –
tangent arcs & parhelia
CO2 – different ice crystal structure
Mars CO2 Atm Ice Simulation
Jupiter ! NH3-rich atmospheres ! Highest clouds, -110oC ! Ammonia forms crystals with cubic symmetry ! Slightly greater index of refraction than for CO2
! NH3-rich atmosphere; ! Crystals form at greater depths in atmosphere
Alien Worlds – Saturn
76
Match the following phenomena to their physical basis (every physical basis may not be
be listed for each phenomenon)
1) Rainbows 2) Supernumerary rainbows 3) Sundogs 4) Opposition brightening
A. 1) reflection 2) refraction 3) refraction and reflection 4) diffraction
B. 1) diffraction 2) refraction 3) refraction 4) shadow enhancement
C. 1) refraction and internal reflection 2) refraction, internal reflection, and diffraction 3) refraction 4) shadow hiding
D. 1) refraction and internal reflection 2) refraction 3) diffraction 4) shadow hiding
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Answer: C 1. In rainbows, internal reflection deflects light at 42°, and
refraction (including dispersion) spreads it into a spectrum
2. Supernumerary rainbows are rainbows, with diffraction by small equally sized water droplets - classical geometric optics doesn’t explain them (but light path in droplets is still like normal rainbows)
3. Sundogs are created by refraction of light through vertically oriented hexagonal ice crystals
4. Opposition brightening occurs when an observer is between a surface and the sun, so surface is seen from the top, and the shadows caused by bumps in the surface are hidden 77