Physics 1C. Lecture 22A. "There are two ways of spreading light: to be the candle or the mirror that reflects it." --Edith Wharton

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Transcription:

Physics 1C Lecture 22A "There are two ways of spreading light: to be the candle or the mirror that reflects it." --Edith Wharton

The Nature of Light An interesting question developed as to the nature of light: if light is indeed a wave then why can it travel from the Sun to Earth when there is no medium present? The answer: Light is a particle (photon), particles do not require a medium. But if light is a particle, then how can it bend around corners? The answer: Light is a wave, waves that propagate outward can bend around an obstacle.

The Nature of Light But, if light is a wave how does that explain the photoelectric effect? The answer: Light is a particle, only particles with high energy can eject the electrons. But if light is a particle, then how does this explain the standing wave pattern I see with interference from double slits? The answer: Light is a wave, waves will create bright/dark spots depending on path length difference.

The Nature of Light But how can light be both a particle and a wave? We say that light can have both wavelike properties and particle-like properties. This is called wave-particle duality. In some experiments light acts as a wave and in others it acts as a particle. Experimenters will find whatever they are testing for. Nature prevents testing both qualities at the same time.

The Nature of Light We can identify light as being particles called photons. Each photon has a particular energy which is quantified by its frequency. E = hf h is called Planck s constant and is: h = 6.63 10 34 J s Note how wave-particle duality is incorporated here, light interacts like a particle with other particles but its energy is for a given frequency like a wave.

The Nature of Light From now on we will have to treat light as having both properties (wave and particle). As light moves through a medium (such as air) it will move in a straight line path. We draw imaginary lines (known as light rays) to represent this path. We can also represent this motion with wave fronts. A wave front is a surface where the wave has the same phase and amplitude.

Ray Model of Light 1) Light rays travel in straight lines in a given medium. 2) Light rays can cross. They do not interact with each other. Two rays can cross without either being affected in any way. 3) A light ray travels forever unless it interacts with matter. It can interact with matter by either: reflection, refraction, scattering or absorption.

Ray Model of Light 4) An object is a source of light rays. Rays originate from every point on the object, and each point sends rays in all directions. If the object is far away, the rays will appear parallel to the observer. We make no distinction between self-luminous objects and reflective objects. 5) The eyes sees by focusing a diverging bundle of rays.

The Nature of Light The incident light ray will move in a straight line path as long as the medium does not change. But, when it encounters a boundary with a second medium, (at least) part of this incident ray is reflected back into the first medium. If the boundary is a smooth surface, the reflection is known as specular reflection. This means all the reflected rays will be parallel to one another.

The Nature of Light If the boundary is a rough surface, the reflection is known as diffuse reflection. This means that the reflected rays will travel in a variety of directions. Diffuse reflection is how you can see most everyday objects. Although diffuse reflection is more common, it is harder to mathematically model than specular reflection.

Law of Reflection We define a normal (perpendicular line to the surface) at the point where the incident ray hits strikes the surface. The incident angle, θ 1, is the angle that the incident ray makes with respect to the normal. The reflected angle, θ 1, is the angle that the reflected ray makes with respect to the normal. The angle of incidence is equal to the angle of reflection. θ 1 = ʹ θ 1

Refraction of Light Also, when an incident ray of light in a medium encounters a boundary with a second medium, part of this incident ray may enter the second medium. The ray that enters the second medium is bent at the boundary. This bending of the ray is called refraction. The incident ray, the reflected ray, the refracted ray, and the normal all lie in the same plane.

Refraction of Light For example, let s look at red laser light incident upon a block of lucite. Ray 1 is called the incident ray Ray 2 is the reflected ray from the air/ lucite boundary. Ray 3 is refracted into the lucite. Ray 4 is the reflected ray from the bottom lucite boundary. Ray 5 is refracted into the air.

Refraction of Light When light passes from one medium to another, it is refracted because the speed of light is different in the two media. The index of refraction, n, of a medium can be defined: n is a unitless ratio For a vacuum, n=1 (exactly). For all other media, n>1.

Indices of Refraction

Frequency Between Media As light travels from one medium to another, its frequency does not change. Both the wave speed and the wavelength do change. The wavefronts do not pile up, nor are created nor destroyed at the boundary, so the frequency must stay the same. λ 1 λ 2 = n 2 n 1

Slow to fast, light bends away from the normal. Snell s Law Fast to slow, light bends towards the normal. Or think of a car axle: one wheel stuck in mud (slow), other wheel on pavement (fast) pivots around. This is the basis for Snell s Law.

Refraction of Light The angle of refraction depends upon the material (by index of refraction) and the angle of incidence: n 1 sinθ 1 = n 2 sinθ 2 where θ 1 is the angle of incidence (30 o in the diagram). θ 2 is the angle of refraction. n 1, n 2 are the indices of refraction of the first and second media, respectively.

Snell s Law For example, for this specific case (air to glass with an incident angle of 30.0 o ): n 1 sinθ 1 = n 2 sinθ 2 sinθ 2 = n 1 sinθ 1 n 2 n θ 2 = sin 1 1 sinθ 1 n 2 1.0003 θ 2 = sin 1 1.52 sin30 θ 2 = sin 1 0.329 ( ) =19.2

Clicker Question 22A-1 A light ray travels from medium 1 to medium 3 as shown in the figure below. What can we say about the relationship between the index of refraction for medium 1 (n 1 ) and the index of refraction for medium 3 (n 3 )? A) n 3 > n 1. B) n 3 = n 1. C) n 3 < n 1. D) We can t compare n 1 to n 3 without knowing n 2.

For Next Time (FNT) Start reading Chapter 22 Finish working on the homework for Chapter 21