Optics Reflection and Refraction Mirrors and Lenses Chapter 17 and 18
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Transcript of Optics Reflection and Refraction Mirrors and Lenses Chapter 17 and 18
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Optics Reflection and Refraction
Mirrors and LensesChapter 17 and 18
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Particles Waves
Light = EM waves
Historical debate on nature of lightor
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Wave-particle dualityQuantum OpticsLasers
Planck / EinsteinMichelson Maiman (Laser)…
What is Light? - Revisited
LASER
Paradoxes in physics (BB radiation/ photoelectric effect)Quantisation of light (photons) E=hνBohr model of atomWavefunctions / ProbabilityDiffraction of electrons
Stimulated emission
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REFLECTION REFRACTION
DIFFRACTION INTERFERENCE
Fundamentals of Optics
Continuum of waves Finite no. of waves
IMAGING
POLARISATION
EM-theory
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Refraction, Reflection, and Diffraction• http://www.acoustics.salford.ac.uk/schools/
teacher/lesson3/flash/whiteboardcomplete.swf
• Reflection – Waves bounce off a surface• Refraction- Waves bend when they pass
through a boundary• Diffraction- Waves spread out (bend) when
they pass through a small opening or move around a barrier.
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Reflection• When a wave encounters a barrier, it can reflect or the bounce
off of the obstacle. • Examples: Light – Mirrors Sound - Echo• Most objects we see reflect light rather than emit their own
light.• Fermat's principle - light travels in straight lines and will take the
path of least time
MIRROR
A B
Wrong Path True Path
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Law of Reflection
• The Law of Reflection states :The angle of incidence equals the angle of reflection. θi = θr
• This is true for both flat mirrors and curved mirrors.
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Specular vs. Diffuse Reflection
• If the Law of Reflection is always observed, why do some objects seem to reflect light better than others?
• In diffuse reflection, waves are reflected in many different ways from a rough surface (you can’t see your refection)
• In specular reflection, waves are reflected in the same direction from a smooth surface (you can see your reflection)
The Law of Reflection is Always Observed (regardless of the orientation of the surface)
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Specular reflection from metal
Diffuse reflection from skin
Calm water can provide for the specular reflection of light from the mountain creating an image of the mountain on the surface of the water.
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Mirror Image
• We trace rays from the object• The image formed by the plane mirror is called a virtual
image• The image is the same distance behind the
mirror as the object is in front of it• The object and the image are the same size
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Refraction• When one medium ends and another begins, that is called a boundary.• When a wave encounters a boundary that is more dense, part of it is
reflected and part of it is transmitted
• The frequency of the wave is not altered when crossing a barrier, but the speed and wavelength are.
• The change in speed and wavelength can cause the wave to bend, if it hits the boundary at an angle other than 90°.
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Refraction for Light Waves• For light waves, this bending as light enters the water can
cause objects under water to appear at a different location than they actually are.
Water
Fish in the water appear closer and nearer the surface.
n – index of refraction: n = speed of light in a vacuum/ speed of light in material
n2= 1.0
n1= 1.33
θ2
θ1
•The index of refraction gives the speed of light in a medium:
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Apparent Depth• The submerged object's apparent depth equals its true depth divided by
the liquid's index of refraction: d' = d(n2/n1). Note: n2 is the index of refraction of the medium above the surface and n1 is the index of refraction of the medium below the surface.
www.physics.gla.ac.uk/~johannes/optics_lecture/overheads03_1_2_4-5.pdf
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Critical Angle• At an interface, when light is going from a region of
high refractive index (lower speed) to lower index (higher speed), the light is bent away from the normal
• If the angle of incidence gets great enough it will be bending away at 90o
• This is called the critical angle
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Total Internal Reflection• Once the angle of incidence is larger than the
critical angle, the light cannot escape the higher index material
• This means that all the light is reflected from the surface back into the higher index material
• This is total internal reflection
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Refraction for Sound Waves• Sound waves bend when passing into cooler or warmer air
because the speed of sound depends on the temperature of the air.
• Sound travels slower in cooler air so the sound waves below are bend toward the surface of the water where the air is cooler.
Refraction for Water WavesWater waves bend when they pass from deep water into shallow water, the wavelength shortens and they slow down.
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Thin Film Interference in Peacocks
• Iridescence of peacock feathers is caused by light reflected from complex layered surface
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Thin Film Interference in Bubbles
• We see colors on clear soap bubbles due to a combination of refraction and interference
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Thin Film Interference
• Rays 1 and 2 interfere• Ray 1 suffers a phase change of 180 degrees
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Non-Reflective Coatings• What must be the thickness t of silicon
oxide for zero reflection of light with a wavelength of 550 nm?
• Since the phase changes cancel, we need a one-half wavelength shift as Ray 2 travels the extra distance 2t:
• Shifted wavelength in SiO: λ’ = λ/n = 550 nm /1.45 = 379.3 nm
• 2t = (1/2)(379.3 nm)• t = 94.8 nm
Note: A half wavelength phase occurs when the reflected rays reflects from a medium with higher index of refraction
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Lenses are used to focus light and form images. There are a variety of possible types; we will consider only the symmetric ones, the double concave and the double convex.
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Converging Lens
Diverging Lens
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A ray diagram uses three rays to find the height and location of the image produced by a lens.
The three principal rays for lenses are similar to those for mirrors:
• The P ray—or parallel ray—approaches the lens parallel to its axis.
• The F ray is drawn toward (concave) or through (convex) the focal point.
• The midpoint ray (M ray) goes through the middle of the lens. Assuming the lens is thin enough, it will not be deflected. This is the thin-lens approximation.
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Ray Tracing for Lenses
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note: C = 2f, where f is the focal point
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The thin-lens approximation and the magnification equation:
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Sign conventions for thin lenses:
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Thin Lens Combination
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Example 1An object is placed 20 cm in front of a converging lens of
focal length 10 cm. Where is the image? Is it upright or inverted? Real or virtual? What is the magnification of the image?
Real image,
magnification = −
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Example 2An object is placed 5 cm in front of a converging lens of focal
length 10 cm. Where is the image? Is it upright or inverted? Real or virtual? What is the magnification of the image?
Virtual image, as viewed from the right, the light appears to be coming from the (virtual) image, and not the object.
Magnification = +2
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Spherical Mirrors
• A spherical mirror has the shape of a section of a sphere. If the outside is mirrored, it is convex; if the inside is mirrored, it is concave.
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Spherical Mirrors
• Spherical mirrors have a central axis (a radius of the sphere) and a center of curvature (the center of the sphere).
Text
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Concave MirrorFor a real object very far away from the mirror, the real image is formed at the focus
For a real object close to the mirror but outside of the center of curvature, the real image is formed between C and f. The image is inverted and smaller than the object.
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For a real object at C, the real image is formed at C. The image is inverted and the same size as the object.
For a real object between C and f, a real image is formed outside of C. The image is inverted and larger than the object
note: C = 2f, where f is the focal point and C is the center of curvature
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For a real object at f, no image is formed. The reflected rays are parallel and never converge.
For a real object between f and the mirror, a virtual image is formed behind the mirror. The position of the image is found by tracing the reflected rays back behind the mirror to where they meet. The image is upright and larger than the object.
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Convex Mirror
For a convex mirror the image from a real object is always behind the mirror, smaller than the object, upright and virtual.
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Summary of Mirrors
•Mirror equation: •Focal length of a convex mirror
•Focal length of a concave mirror
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Here are the sign conventions for concave and convex mirrors:
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Example 1An object is placed 30 cm in front of a concave mirror of radius 10
cm. Where is the image located? Is it real or virtual? Is it upright or inverted? What is the magnification of the image?
di>0 Real Image
m = − di / do = −1/5
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Example 2An object is placed 3 cm in front of a concave mirror of radius 20
cm. Where is the image located? Is it real or virtual? Is it upright or inverted? What is the magnification of the image?
Virtual image, di <0
Magnified, |m| > 1,
not inverted. m > 0
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Diffraction• Diffraction involves a change in direction of waves as they
pass through an opening or around a barrier in their path.
• http://www.ngsir.netfirms.com/englishhtm/Diffraction.htm
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Diffraction of Sound and Light Waves
Sound waves bend around obstacles and bend when passing through an opening making it possible to hear sound outside an open door or behind an obstacle.
Light waves also bend around obstacles and when passing through an opening creating a diffraction pattern on a screen.
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Sources
• http://www.physics.mun.ca/~jjerrett/lenses/convex.html
• http://www.educypedia.be/education/physicsopticslenses.htm
• pls.atu.edu/physci/physics/people/bullock/Physical_principles_2/Lectures/Chapter_26.ppt
• www.physics.umd.edu/courses/Phys263/wth/fall04/downloads/LectureNotes/