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Optics
Reflection & Refraction
Optical Systems
Spring 2006
UCSD: Physics 8; 2006
2
Reflection
• We describe the path of light as straight-line rays
– “geometrical optics” approach
• Reflection off a flat surface follows a simple rule:
– angle in (incidence) equals angle out
– angles measured from surface “normal” (perpendicular)
surface normal
same
angle
incident ray exit ray
Spring 2006
UCSD: Physics 8; 2006
3
Reflection, continued
• Also consistent with “principle of least time”
– If going from point A to point B, reflecting off a mirror, the
path traveled is also the most expedient (shortest) route
A
B
too long
shortest path;
equal angles
Spring 2006
UCSD: Physics 8; 2006
4
Hall Mirror
• Useful to think in terms of images
“image” you
“real” you
mirror only
needs to be half as
high as you are tall. Your
image will be twice as far from you
as the mirror.
Spring 2006
UCSD: Physics 8; 2006
5
Curved mirrors
• What if the mirror isn’t flat?
– light still follows the same rules, with local surface normal
• Parabolic mirrors have exact focus
– used in telescopes, backyard satellite dishes, etc.
– also forms virtual image
Spring 2006
UCSD: Physics 8; 2006
6
Refraction
• Light also goes through some things
– glass, water, eyeball, air
• The presence of material slows light’s progress
– interactions with electrical properties of atoms
• The “light slowing factor” is called the index of refraction
– glass has n = 1.52, meaning that light travels about 1.5 times
slower in glass than in vacuum
– water has n = 1.33
– air has n = 1.00028
– vacuum is n = 1.00000 (speed of light at full capacity)
Spring 2006
UCSD: Physics 8; 2006
7
n2 = 1.5
n1 = 1.0
A
B
Refraction at a plane surface
• Light bends at interface between refractive indices
– bends more the larger the difference in refractive index
– can be effectively viewed as a “least time” behavior
• get from A to B faster if you spend less time in the slow medium
1
2
Experts only:
n1sin1 = n2sin2
Spring 2006
UCSD: Physics 8; 2006
8
Driving Analogy
• Let’s say your house is 12 furlongs off the road in the
middle of a huge field of dirt
– you can travel 5 furlongs per minute on the road, but only 3
furlongs per minute on the dirt
• this means “refractive index” of the dirt is 5/3 = 1.667
– Starting from point A, you want to find the quickest route:
• straight across (AD)—don’t mess with the road
• right-angle turnoff (ABD)—stay on road as long as possible
• angled turnoff (ABD)—compromise between the two
A B C
D (house)
leg dist. t@5 t@3
AB 5 1 —
AC 16 3.2 —
AD 20 — 6.67
BD 15 — 5
CD 12 — 4
road
dirt
AD: 6.67 minutes
ABD: 6.0 minutes: the optimal path is a “refracted” one
ACD: 7.2 minutes
Note: both right triangles in figure are 3-4-5
Spring 2006
UCSD: Physics 8; 2006
9
Total Internal Reflection
• At critical angle, refraction no longer occurs
– thereafter, you get total internal reflection
– for glass, the critical internal angle is 42°
– for water, it’s 49°
– a ray within the higher index medium cannot escape at
shallower angles (look at sky from underwater…)
n2 = 1.5
n1 = 1.0
42°
incoming ray hugs surface
Spring 2006
UCSD: Physics 8; 2006
10
Refraction in Suburbia
• Think of refraction as a pair of wheels on an axle
going from sidewalk onto grass
– wheel moves slower in grass, so the direction changes
Note that the wheels
move faster (bigger space)
on the sidewalk, slower
(closer) in the grass
Spring 2006
UCSD: Physics 8; 2006
11
Even gets Total Internal Reflection Right
• Moreover, this analogy is mathematically equivalent
to the actual refraction phenomenon
– can recover Snell’s law: n1sin1 = n2sin2
Wheel that hits sidewalk starts to go faster,
which turns the axle, until the upper wheel
re-enters the grass and goes straight again
Spring 2006
UCSD: Physics 8; 2006
12
Questions
• What do you think you would see from underwater looking
up at sky?
• Why do the sides of aquariums look like mirrors from the
front, but like ordinary glass from the sides?
• If you want to spear a fish from above the water, should
you aim high, right at the fish, or aim low (assume the fish
won’t move)?
Spring 2006
UCSD: Physics 8; 2006
13
n1 = 1.5 n2 = 1.0
Reflections, Refractive offset
• Let’s consider a thick piece of glass (n = 1.5), and the
light paths associated with it
– reflection fraction = [(n1 – n2)/(n1 + n2)]2
– using n1 = 1.5, n2 = 1.0 (air), R = (0.5/2.5)2 = 0.04 = 4%
incoming ray
(100%)
96%
92% transmitted
0.16%
4%
4%
8% reflected in two
reflections (front & back)
image looks displaced
due to jog
Spring 2006
UCSD: Physics 8; 2006
14
Let’s get focused…
• Just as with mirrors, curved lenses follow same rules
as flat interfaces, using local surface normal
A lens, with front and back curved surfaces, bends
light twice, each diverting incoming ray towards
centerline.
Follows laws of refraction at each surface.
Parallel rays, coming, for instance from a specific
direction (like a distant bird) are focused by a convex
(positive) lens to a focal point.
Placing film at this point would record an image of
the distant bird at a very specific spot on the film.
Lenses map incoming angles into positions in the
focal plane.
Spring 2006
UCSD: Physics 8; 2006
15
Cameras, in brief
In a pinhole camera, the hole is so small that light hitting any particular point
on the film plane must have come from a particular direction outside the camera
In a camera with a lens, the same applies: that a point on the film plane
more-or-less corresponds to a direction outside the camera. Lenses have
the important advantage of collecting more light than the pinhole admits
pinhole
image at
film plane
object
image at
film plane
object
lens
Spring 2006
UCSD: Physics 8; 2006
16
The Eye
• Now for our cameras…
• Eye forms image on retina, where light is sensed
– Cornea does 80% of the work, with the lens providing slight
tweaks (accommodation, or adjusting)
Refractive indices:
air: 1.0
cornea: 1.376
fluid: 1.336
lens: 1.396
Central field of view (called fovea)
densely plastered with receptors for
high resolution & acuity. Fovea only
a few degrees across.
Spring 2006
UCSD: Physics 8; 2006
17
Questions
• Why are contacts and corneal surgery (e.g., radial
keratotomy) as effective as they are without messing
with innards of eye?
• Why can’t we focus our eyes under water?
• Why do goggles help?
Spring 2006
UCSD: Physics 8; 2006
18
References and Assignments
• References
– www.education.eth.net/acads/physics/light-VIII.htm
• lenses, etc.
– www.howstuffworks.com/camera.htm?printable=1
• cameras
• Assignments
– Q/O #4 due Friday, 5/26 at 6PM
– HW #7 (due 06/01): TBA
• Think up topics you’d like to see covered before the
end of the quarter
– use the WebCT discussion board to contribute ideas
– or e-mail me

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16_optics_r (1).ppt

  • 2. Spring 2006 UCSD: Physics 8; 2006 2 Reflection • We describe the path of light as straight-line rays – “geometrical optics” approach • Reflection off a flat surface follows a simple rule: – angle in (incidence) equals angle out – angles measured from surface “normal” (perpendicular) surface normal same angle incident ray exit ray
  • 3. Spring 2006 UCSD: Physics 8; 2006 3 Reflection, continued • Also consistent with “principle of least time” – If going from point A to point B, reflecting off a mirror, the path traveled is also the most expedient (shortest) route A B too long shortest path; equal angles
  • 4. Spring 2006 UCSD: Physics 8; 2006 4 Hall Mirror • Useful to think in terms of images “image” you “real” you mirror only needs to be half as high as you are tall. Your image will be twice as far from you as the mirror.
  • 5. Spring 2006 UCSD: Physics 8; 2006 5 Curved mirrors • What if the mirror isn’t flat? – light still follows the same rules, with local surface normal • Parabolic mirrors have exact focus – used in telescopes, backyard satellite dishes, etc. – also forms virtual image
  • 6. Spring 2006 UCSD: Physics 8; 2006 6 Refraction • Light also goes through some things – glass, water, eyeball, air • The presence of material slows light’s progress – interactions with electrical properties of atoms • The “light slowing factor” is called the index of refraction – glass has n = 1.52, meaning that light travels about 1.5 times slower in glass than in vacuum – water has n = 1.33 – air has n = 1.00028 – vacuum is n = 1.00000 (speed of light at full capacity)
  • 7. Spring 2006 UCSD: Physics 8; 2006 7 n2 = 1.5 n1 = 1.0 A B Refraction at a plane surface • Light bends at interface between refractive indices – bends more the larger the difference in refractive index – can be effectively viewed as a “least time” behavior • get from A to B faster if you spend less time in the slow medium 1 2 Experts only: n1sin1 = n2sin2
  • 8. Spring 2006 UCSD: Physics 8; 2006 8 Driving Analogy • Let’s say your house is 12 furlongs off the road in the middle of a huge field of dirt – you can travel 5 furlongs per minute on the road, but only 3 furlongs per minute on the dirt • this means “refractive index” of the dirt is 5/3 = 1.667 – Starting from point A, you want to find the quickest route: • straight across (AD)—don’t mess with the road • right-angle turnoff (ABD)—stay on road as long as possible • angled turnoff (ABD)—compromise between the two A B C D (house) leg dist. t@5 t@3 AB 5 1 — AC 16 3.2 — AD 20 — 6.67 BD 15 — 5 CD 12 — 4 road dirt AD: 6.67 minutes ABD: 6.0 minutes: the optimal path is a “refracted” one ACD: 7.2 minutes Note: both right triangles in figure are 3-4-5
  • 9. Spring 2006 UCSD: Physics 8; 2006 9 Total Internal Reflection • At critical angle, refraction no longer occurs – thereafter, you get total internal reflection – for glass, the critical internal angle is 42° – for water, it’s 49° – a ray within the higher index medium cannot escape at shallower angles (look at sky from underwater…) n2 = 1.5 n1 = 1.0 42° incoming ray hugs surface
  • 10. Spring 2006 UCSD: Physics 8; 2006 10 Refraction in Suburbia • Think of refraction as a pair of wheels on an axle going from sidewalk onto grass – wheel moves slower in grass, so the direction changes Note that the wheels move faster (bigger space) on the sidewalk, slower (closer) in the grass
  • 11. Spring 2006 UCSD: Physics 8; 2006 11 Even gets Total Internal Reflection Right • Moreover, this analogy is mathematically equivalent to the actual refraction phenomenon – can recover Snell’s law: n1sin1 = n2sin2 Wheel that hits sidewalk starts to go faster, which turns the axle, until the upper wheel re-enters the grass and goes straight again
  • 12. Spring 2006 UCSD: Physics 8; 2006 12 Questions • What do you think you would see from underwater looking up at sky? • Why do the sides of aquariums look like mirrors from the front, but like ordinary glass from the sides? • If you want to spear a fish from above the water, should you aim high, right at the fish, or aim low (assume the fish won’t move)?
  • 13. Spring 2006 UCSD: Physics 8; 2006 13 n1 = 1.5 n2 = 1.0 Reflections, Refractive offset • Let’s consider a thick piece of glass (n = 1.5), and the light paths associated with it – reflection fraction = [(n1 – n2)/(n1 + n2)]2 – using n1 = 1.5, n2 = 1.0 (air), R = (0.5/2.5)2 = 0.04 = 4% incoming ray (100%) 96% 92% transmitted 0.16% 4% 4% 8% reflected in two reflections (front & back) image looks displaced due to jog
  • 14. Spring 2006 UCSD: Physics 8; 2006 14 Let’s get focused… • Just as with mirrors, curved lenses follow same rules as flat interfaces, using local surface normal A lens, with front and back curved surfaces, bends light twice, each diverting incoming ray towards centerline. Follows laws of refraction at each surface. Parallel rays, coming, for instance from a specific direction (like a distant bird) are focused by a convex (positive) lens to a focal point. Placing film at this point would record an image of the distant bird at a very specific spot on the film. Lenses map incoming angles into positions in the focal plane.
  • 15. Spring 2006 UCSD: Physics 8; 2006 15 Cameras, in brief In a pinhole camera, the hole is so small that light hitting any particular point on the film plane must have come from a particular direction outside the camera In a camera with a lens, the same applies: that a point on the film plane more-or-less corresponds to a direction outside the camera. Lenses have the important advantage of collecting more light than the pinhole admits pinhole image at film plane object image at film plane object lens
  • 16. Spring 2006 UCSD: Physics 8; 2006 16 The Eye • Now for our cameras… • Eye forms image on retina, where light is sensed – Cornea does 80% of the work, with the lens providing slight tweaks (accommodation, or adjusting) Refractive indices: air: 1.0 cornea: 1.376 fluid: 1.336 lens: 1.396 Central field of view (called fovea) densely plastered with receptors for high resolution & acuity. Fovea only a few degrees across.
  • 17. Spring 2006 UCSD: Physics 8; 2006 17 Questions • Why are contacts and corneal surgery (e.g., radial keratotomy) as effective as they are without messing with innards of eye? • Why can’t we focus our eyes under water? • Why do goggles help?
  • 18. Spring 2006 UCSD: Physics 8; 2006 18 References and Assignments • References – www.education.eth.net/acads/physics/light-VIII.htm • lenses, etc. – www.howstuffworks.com/camera.htm?printable=1 • cameras • Assignments – Q/O #4 due Friday, 5/26 at 6PM – HW #7 (due 06/01): TBA • Think up topics you’d like to see covered before the end of the quarter – use the WebCT discussion board to contribute ideas – or e-mail me

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