Outline The Refraction of Light Forming Images with a Plane Mirror 26-3 Spherical Mirror 26-4 Ray Tracing and the Mirror Equation

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Chapter 6 Geometrical Optics Outline 6-1 The Reflection of Light 6- Forming Images with a Plane Mirror 6-3 Spherical Mirror 6-4 Ray Tracing and the Mirror Equation 6-5 The Refraction of Light 6-6 Ray Tracing for Lens 6-7 Thin Lens Equation

6-5 The Refraction of Light Refraction: Light will change the motion direction when it travels from one medium to the other. This phenomenon is called refraction. Definition of the index of refraction in a medium, n >=1 n = v c ( 6 10) Where, v is the speed in the medium. C is the speed in vacuum. Refraction is caused by the difference of speeds in two mediums!

Derive the Snell s law (refraction law): n sinθ = n sinθ 1 1 For the green and grey triangles, for the same wave-front we have sinθ v Δt AB v Δt AB 1 1 =, sinθ =, Combining these two eqs, we have sinθ 1 sinθ = v v 1 Figure 6-1 The Basic Mechanism of Refraction

That is, sinθ 1 sinθ = ( c / n ) ( c / n ) ( 1 n Snell s Law (Refraction Law) n1 sinθ1 = n sinθ (6 11) Exercise 6-4 A beam of light in air enter (a) water (n= 1.33) or (b) glass (n= 1.50) at an angle of 60º relative to the normal. Find the angles of refraction for each case.

Example 6-8 Prism Dispersion, and Rainbow

Total Internal Reflection The angel of total internal reflection can be calculated as (when n 1 > n ): n c = 1 sinθ = n sin 90 n Figure 6 5 Figure 6-5 Total Internal Reflection

Critical Angle for Total Internal Reflection, θ c sinθ = n (6 1) c n 1 Note: 1) n 1 >n ) Total internal reflection happens when θ i >= θ c 3) 100% reflection for total internal reflection: no light loss

An example of total internal reflection Figure 6-6 Prisms and Binocular

Example 6-6 Find the critical angle for light traveling from glass (n=1.50) to (a) air (n=1.00), and (b) water (n=1.33). Solution: Part (a) n 1.0 sin θc = =, θc = 41.5 n 1 150 1.50 Part (b) n 1.33 = = = sin θc, θc 6.5 n 1 1.50

Total Polarization Light reflected from a nonmetallic surface is generally polarized to some degree. At a special angle of incidence, Brewster s angle, θ B is : Complete Polarized reflection: Reflected light is completely polarized when the refracted beams are at a right angle with the reflection beam. The direction of polarization is parallel to the reflection surface. Figure 6-8 gu e 6 8 Brewster s Angle note the 90º at Brewster angle

Derive of Brewster s angle: According to Snell s Law, n1 sinθ B= n sinθ ( a) Also, for complete polarization reflection, we have θ B + 90 + θ = 180 ; that is θ B + θ = 90 therefore, sinθ = sin(90 θ ) = B cosθ B ( b) Combining (a) and (b), we have Brewster s Angle, θ B n tan = (6 13) n θ B n 1

Exercise 6-5 Find the Brewster s angle for light reflected in the air from the top of glass (n= 1.50) coffee table.

6-6 Ray Tracing for Lenses (Find the image position) Lens: a lens is a piece of glass or other transparent material that converges or diverges the light beams for imaging purpose. Two kinds of lenses: Converging lens and Diverging lens (identifying by comparing the thicknesses of the center and edge) Fi 6 9 Figure 6-9 A Variety of Converging and Diverging Lenses

Figure 6-30 A Converging lens Lens Compared with a Pair of Prisms f Figure 6-31 A Diverging Lens Compared with a Pair of Prisms f

Ray Tracing The P ray: the parallel ray. It is parallel to the principle axis and will pass the focal point of a lens (or extended line will pass the focus point). The F ray: the ray that pass the focus point of a lens (or extended line pass the focus point). It is parallel to principle axis after going through the lens. The midpoint Ray (M ray): the ray that go through the middle of a lens. It is a straight line for a thin lens. Rays can be inversed!!! Figure 6-3 The Three Principal Rays Used for Ray Tracing with Converging Lenses f

Figure 6-33 The Three Principal Rays Used for Ray Tracing with Diverging i Lenses f

Figure 6-34 The Image Formed by a Diverging (Concave) Lens Virtual image!

Figure 6-35 Ray Tracing for a Convex Lens: Object at different distances. Real image! Virtual image!

Snell s Law (Refraction Law) Summary n1 sinθ1 = n sinθ (6 11) Critical Angle for Total Internal Reflection, θ c sin = n (6 1) θ c n 1 Brewster s Angle, θ B tan θ B n = (6 13) n 1 Ray Tracing (find the image position): The P ray: the parallel ray. It is the parallel to the principle axis and will pass the focal point of a lens. The F ray: the ray that pass the focus point of a lens. The midpoint Ray (M ray): the ray that go through the middle of a lens.