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Chapter 27 Interference and the Wave Nature of Light
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Chapter 27

Jan 17, 2016

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Chapter 27. Interference and the Wave Nature of Light. 27.1 The Principle of Linear Superposition. When two or more light waves pass through a given point, their electric fields combine according to the principle of superposition. - PowerPoint PPT Presentation
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Page 1: Chapter 27

Chapter 27

Interference and the Wave Nature of Light

Page 2: Chapter 27

27.1 The Principle of Linear Superposition

When two or more light waves pass through a given point, their electricfields combine according to the principle of superposition.

The waves emitted by the sources start out in phase and arrive at point P in phase, leading to constructive interference.

,3,2,1,0 12 mm

Page 3: Chapter 27

27.1 The Principle of Linear Superposition

The waves emitted by the sources start out in phase and arrive at point P out of phase, leading to destructive interference.

,3,2,1,0 21

12 mm

Page 4: Chapter 27

27.1 The Principle of Linear Superposition

If constructive or destructive interference is to continue ocurring at a point, the sources of the waves must be coherent sources.

Two sources are coherent if the waves they emit maintain a constantphase relation.

Page 5: Chapter 27

27.2 Young’s Double Slit Experiment

In Young’s experiment, two slits acts as coherent sourcesof light.

Light waves from these slits interfere constructively anddestructively on the screen.

Page 6: Chapter 27

27.2 Young’s Double Slit Experiment

The waves coming from the slits interfere constructively ordestructively, depending on the difference in distances betweenthe slits and the screen.

Page 7: Chapter 27

27.2 Young’s Double Slit Experiment

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Bright fringes of a double-slit

Dark fringes of a double-slit

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m

,3,2,1,0 sin 21 md

m

Page 8: Chapter 27

27.2 Young’s Double Slit Experiment

Example 1 Young’s Double-Slit Experiment

Red light (664 nm) is used in Young’s experiment with slits separatedby 0.000120 m. The screen is located a distance 2.75 m from the slits.Find the distance on the screen between the central bright fringe andthe third-order bright fringe.

Page 9: Chapter 27

27.2 Young’s Double Slit Experiment

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Page 10: Chapter 27

27.2 Young’s Double Slit Experiment

Conceptual Example 2 White Light and Young’s Experiment

The figure shows a photograph that illustrates the kind of interferencefringes that can result when white light is used in Young’s experiment.Why does Young’s experiment separate white light into its constituent colors? In any group of colored fringes, such as the two singled out, why is red farther out from the central fringe than green is? Why isthe central fringe white?

Page 11: Chapter 27

27.3 Thin Film Interference

Page 12: Chapter 27

27.3 Thin Film Interference

Because of reflection and refraction,two light waves enter the eye when lightshines on a thin film of gasoline floating on a thick layer of water.

Because of the extra distance traveled, therecan be interference between the two waves.

nvacuum

film

Page 13: Chapter 27

27.3 Thin Film Interference

When light travels through a material witha smaller refractive index towards a materialwith a larger refractive index, reflection atthe boundary occurs along with a phasechange that is equivalent to one-half ofa wavelength in the film.

When light travels from a larger towards a smaller refractive index, there is no phasechange upon reflection.

Page 14: Chapter 27

27.3 Thin Film Interference

Example 3 A Colored Thin Film of Gasoline

A thin film of gasoline floats on a puddle of water. Sunlight falls perpendicularly on the film and reflects into your eyes. The film hasa yellow hue because destructive interference eliminates the colorof blue (469 nm) from the reflected light. The refractive indices of theblue light in gasoline and water are 1.40 and 1.33. Determine the minimum non-zero thickness of the film.

Page 15: Chapter 27

27.3 Thin Film Interference

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Condition for destructive interference

Page 16: Chapter 27

27.3 Thin Film Interference

Conceptual Example 4 Multicolored Thin Films

Under natural conditions, thin films, like gasoline on water or likethe soap bubble in the figure, have a multicolored appearance that oftenchanges while you are watching them. Why are such films multicoloredand why do they change with time?

Page 17: Chapter 27

27.3 Thin Film Interference

The wedge of air formed between two glass platescauses an interferencepatter of alternating darkand bright fringes.

Page 18: Chapter 27

27.3 Thin Film Interference

Page 19: Chapter 27

27.4 The Michelson Interferometer

A schematic drawing ofa Michelson interferometer.

Page 20: Chapter 27

27.5 Diffraction

Diffraction is the bending of waves aroundobstacles or the edges of an opening.

Huygens’ principle

Every point on a wave front acts as a sourceof tiny wavelets that move forward with the samespeed as the wave; the wave front at a latterinstant is the surface that is tangent to thewavelets.

Page 21: Chapter 27

27.5 Diffraction

The extent of the diffraction increases as the ratio of the wavelengthto the width of the opening increases.

Page 22: Chapter 27

27.5 Diffraction

Page 23: Chapter 27

27.5 Diffraction

This top view shows five sources of Huygens’ wavelets.

Page 24: Chapter 27

27.5 Diffraction

These drawings show how destructiveinterference leads to the first dark fringeon either side of the central bright fringe.

Dark Fringes for a single-slit diffraction

... 3, 2, ,1 sin mw

m

Page 25: Chapter 27

27.5 Diffraction

Page 26: Chapter 27

27.6 Resolving Power

Three photographs of an automobile’s headlights, taken atprogressively greater distances.

Page 27: Chapter 27

27.6 Resolving Power

First minimum of a circular diffraction pattern

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22.1sin

diameter of hole

Page 28: Chapter 27

27.6 Resolving Power

Rayleigh Criterion:

Two point objects are just resolved when the first dark fringe in the diffraction pattern of one falls directly on the central bright fringe in the diffraction pattern of the other.

rad)in ( 22.1 minmin D

Page 29: Chapter 27

27.6 Resolving Power

Conceptual Example 8 What You See is Not What You Get

The French postimpressionist artist Georges Seurat developed atechnique of painting in which dots of color are placed close togetheron the canvas. From sufficiently far away the individual dots are notdistinguishable, and the images in the picture take on a more normalappearance.

Why does the camera resolve the dots, while his eyes do not?

Page 30: Chapter 27

27.7 The Diffraction Grating

An arrangement consisting of a large number of closely spaced,parallel slits is called a diffraction grating.

Page 31: Chapter 27

27.7 The Diffraction Grating

The conditions shown here lead to the first- and second-order intensitymaxima in the diffraction pattern.

Page 32: Chapter 27

27.7 The Diffraction Grating

The bright fringes produced bya diffraction grating are much narrower than those produced bya double slit.

Principal maxima of adiffraction grating

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m

distance betweenslits

Page 33: Chapter 27

27.7 The Diffraction Grating

Example 9 Separating Colors With a Diffraction Grating

A mixture of violet (410 nm) light and red (660 nm) light falls ontoa grating that contains 1.0x104 lines/cm. For each wavelength,find the angle that locates the first-order maximum.

Page 34: Chapter 27

27.7 The Diffraction Grating

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Page 35: Chapter 27

27.8 Compact Discs, Digital Video Discs, and the Use of Interference

Page 36: Chapter 27

27.8 Compact Discs, Digital Video Discs, and the Use of Interference

Page 37: Chapter 27

27.9 X-Ray Diffraction

Page 38: Chapter 27

27.9 X-Ray Diffraction