Changing the Phase of a Light Wave. A light wave travels a distance L through a material of refractive index n. By how much has its phase changed?

Slides:



Advertisements
Similar presentations
Interference in Thin Films
Advertisements

Chapter 9 Light as a Wave.
Another example of interference that is often observed is interference from a thin film. Light incident on the surface of a thin film is reflected from.
Net vibration at point P:
AP Physics Mr. Jean March 30 th, The plan: Review of slit patterns & interference of light particles. Quest Assignment #2 Polarizer More interference.
General Properties of Waves
Chapter 24 Wave Optics.
Electrons as Waves.
Lecture 12 Light: Reflection and Refraction Chapter 22.1  22.4 Outline History of Studies of Light Reflection of Light The Law of Refraction. Index of.
Chapter 15 - Waves Traveling Waves –Types –Classification –Harmonic Waves –Definitions –Direction of Travel Speed of Waves Energy of a Wave Standing Waves.
Interference Physics 202 Professor Lee Carkner Lecture 24.
Interference Physics 202 Professor Lee Carkner Lecture 24.
Chapter Eleven Wave Motion. Light can be considered wavelike by experimental analogies to the behavior of water waves. Experiments with fundamental particles,
c = km/sec I F = I 0 x (cosθ) 2.
Interference in One Dimension
Waves in One dimension. A wave medium is an object, each of whose points can undergo simple harmonic motion (SHM). Examples: 1. A string. Each little.
Chapter 35 Serway & Jewett 6th Ed..
Bending and Bouncing Light Standing Waves, Reflection, and Refraction.
Chapter 37 Wave Optics. Wave optics is a study concerned with phenomena that cannot be adequately explained by geometric (ray) optics.  Sometimes called.
1 Optical Properties of Materials … reflection … refraction (Snell’s law) … index of refraction Index of refraction Absorption.
Aim: What happens to the speed of light in different mediums? Do Now: What is the wavelength of yellow light? v = f λ c = f λ 3 x 10 8 m/s = (5.20 x 10.
Science Physics Definition Test. What is the definition of 1.Scalar 2.Vector 3.Uniform acceleration 4.Velocity 5.Mass 6.Weight 7.Gravitational field 8.Gravitational.
& Electromagnetic Waves.  equivalent to Coulomb’s law.
Phase Change on Reflection To understand interference caused by multiple reflections it is necessary to consider what happens when a light wave moving.
Refraction   Refraction   When light bends as it passes from one material to another due to a change in speed Optical illusions 9/13/2015APHY1011.
Introduction to Light IN THIS LECTURE –Reflection and refraction –Index of refraction –Snell’s Law –Critical Angle –Dispersion and refractive index –Interference.
Sound of Music Learning check! #2. 1. What is the approximate value of the refractive index of glass? A. 1.3 B C D. 133.
Waves Topic 4.5 Wave Properties. Wave Behaviour v Reflection in one dimension.
Waves Waves. Types of Waves l Longitudinal: The medium oscillates in the same direction as the wave is moving è Sound l Transverse: The medium oscillates.
Refraction. As the speed of light is reduced in the slower medium, the wavelength is shortened proportionately. The frequency is unchanged; it is a characteristic.
Resonant motion: amplitude and phase. What resonances to electrons in atoms have?
Interference Patterns Constructive interference occurs at the center point The two waves travel the same distance –Therefore, they arrive in phase.
Interference Patterns Constructive interference occurs at the center point The two waves travel the same distance –Therefore, they arrive in phase.
INTERFERENCE DIVISION OF AMPLITUDE. Interference of waves occurs when waves overlap. There are two ways to produce an interference pattern for light:
Optics II----by Dr.H.Huang, Department of Applied Physics
Lecture Nine: Interference of Light Waves: I
Lecture 24 Interference of Light.
 The behavior of a wave is greatly influenced by the medium in which it is traveling.  The wave frequency remains unchanged in different medium.  The.
Physics 1C Lecture 27A. Interference Treating light as a particle (geometrical optics) helped us to understand how images are formed by lenses and mirrors.
Physics 213 General Physics Lecture Last Meeting: Electromagnetic Waves, Maxwell Equations Today: Reflection and Refraction of Light.
1 Reading: Main 9.0, 9.1, 9.3 GEM 9.1.1, Knight Ch 20 BASIC WAVE CONCEPTS.
Unit 9 Notes Waves.
Lecture 16 Interference Chapter 24.1  24.4 Outline Conditions for Interference Experiments Showing Interference Interference in Thin Films.
Refraction The bending of light due to a change in speed.
Year 1 Science 6.P.1.1. What are waves? “Moving energy” Formed when a force causes vibrations through space or matter Vibrations form wavelike disturbances.
Refraction. Have you ever seen this? Refraction of Light When light travels through a surface between two different media, the light will be refracted.
Amplitude The max. distance the particles move from the “rest position” to: The more energy a wave has → The greater its amplitude Compression or rarefaction.
 .  ’’ a    a    ’ + a = 90 Therefore:   =   ’  
1.To look further at refraction maths 2.To understand dispersion Book Reference : Pages
Holt Physics Chapter 12 Waves Periodic Motion A repeated motion that is back and forth over the same path.
Power Functions…. Definition: Some common power functions…
Q14.Wave Motion. 1.The displacement of a string carrying a traveling sinusoidal wave is given by 1. v 0 /  y 0 2.  y 0 / v 0 3.  v 0 / y 0 4. y.
Refraction And you.
Interference of Light Waves
GROUP DELAY Group delay per unit length can be defined as:
Optics: Refraction 3 Learning Objectives
Waves Review & Electromagnetic Waves Introduction
Purdue University, Physics 220
Electromagnetic Waves
Interference and Diffraction
Today’s agenda: Thin Film Interference.
Waves © D Hoult 2007.
Interference of Light Waves
Complex numbers/phasors and amplitudes
Longitudinal-particles move parallel to wave motion
Optical properties of a conductor
Unit: Sound and Light Lesson 2: Properties of Waves
Energy that can travel directly through space in the form of waves.
Index of Refraction.
Presentation transcript:

Changing the Phase of a Light Wave

A light wave travels a distance L through a material of refractive index n. By how much has its phase changed?

A light wave travels a distance L in vacuum. By how much has its phase changed?

How does the amplitude depend on distance?

A light wave travels a distance L in vacuum. By how much has its phase changed? How does the amplitude depend on distance? At a fixed time, E(x,t) = sin(kx + constant)

E(x 1,t) = sin(k x 1 + constant) E(x 2,t) = sin(k x 2 + constant)

E(x 1,t) = sin(k x 1 + constant) E(x 2,t) = sin(k x 2 + constant) Phase of wave at x 1 = k x 1 + constant Phase of wave at x 2 = k x 2 + constant

E(x 1,t) = sin(k x 1 + constant) E(x 2,t) = sin(k x 2 + constant) Phase of wave at x 1 = k x 1 + constant Phase of wave at x 2 = k x 2 + constant Phase difference = k x 2 - k x 1 = k ( x 2 – x 1 ) = k L

E(x 1,t) = sin(k x 1 + constant) E(x 2,t) = sin(k x 2 + constant) Phase of wave at x 1 = k x 1 + constant Phase of wave at x 2 = k x 2 + constant Phase difference = k x 2 - k x 1 = k ( x 2 – x 1 ) = k L k = 2 B / 8, so that phase difference = 2 B L/ 8

Coming back to our original problem, we can say that the phase change the light undergoes in traveling a distance L through the material is 2 B L / (wavelength of light in material)

Coming back to our original problem, we can say that the phase change the light undergoes in traveling a distance L through the material is 2 B L / (wavelength of light in material) What is the wavelength of light in the material?

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material 8 0 f 0 = c 8 m f m = v

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material 8 0 f 0 = c 8 m f m = v ( 8 0 f 0 ) / ( 8 m f m ) = c / v = n

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material 8 0 f 0 = c 8 m f m = v ( 8 0 f 0 ) / ( 8 m f m ) = c / v = n f 0 = f m

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material 8 0 f 0 = c 8 m f m = v ( 8 0 f 0 ) / ( 8 m f m ) = c / v = n f 0 = f m Therefore, 8 0 / 8 m = n

8 0 = wavelength of light in vacuum 8 m = wavelength of light in material 8 0 f 0 = c 8 m f m = v ( 8 0 f 0 ) / ( 8 m f m ) = c / v = n f 0 = f m Therefore, 8 0 / 8 m = n Or, 8 m = 8 0 / n

The phase has changed by 2 B L / 8 m

= 2 B L / ( 8 0 / n) = 2 B n L / 8 0

The phase has changed by 2 B L / 8 m = 2 B L / ( 8 0 / n) = 2 B n L / 8 0 In traveling a distance L in the material, the wave changes its phase by the same amount that it would have changed if it had traveled a distance n L in vacuum.

The phase has changed by 2 B L / 8 m = 2 B L / ( 8 0 / n) = 2 B n L / 8 0 In traveling a distance L in the material, the wave changes its phase by the same amount that it would have changed if it had traveled a distance n L in vacuum. n L is defined as the optical path length.

How do we represent a phase change mathematically? In free space, the amplitude function is E (x,t) = E 0 exp[i(kx- j t + N )] At a fixed time this is E = A e ikx where A = E 0 exp[i(- j t + N )] The wave amplitude at x 1 is The wave amplitude at x 2 is If E is the complex amplitude at the entry-face of the material, the complex amplitude at the exit face is E exp[i(phase change)] = E exp[2 B i n L / 8 0 ]