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Chapter 27 Interference and the Wave Nature of Light
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Chapter 27 Interference and the Wave Nature of Light.

Dec 27, 2015

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Victoria Knight
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Page 1: Chapter 27 Interference and the Wave Nature of Light.

Chapter 27

Interference and the Wave Nature of Light

Page 2: 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 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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

27.2 Young’s Double Slit Experiment

Page 8: Chapter 27 Interference and the Wave Nature of Light.

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

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m

Page 9: Chapter 27 Interference and the Wave Nature of Light.

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 10: Chapter 27 Interference and the Wave Nature of Light.

27.2 Young’s Double Slit Experiment

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Page 11: Chapter 27 Interference and the Wave Nature of Light.

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 12: Chapter 27 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

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 Interference and the Wave Nature of Light.

27.3 Thin Film Interference

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Page 16: Chapter 27 Interference and the Wave Nature of Light.

27.3 Thin Film Interference

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

Page 17: Chapter 27 Interference and the Wave Nature of Light.

Example• a) Assuming that green light

(λvacuum = 552 nm) strikes the glass plates nearly perpendicularly determine the number of bright fringes that occur between the place where the plates touch and the edge of the sheet of paper (thickness = 4.10 × 10–5 m). (b) Explain why there is a dark fringe where the plates touch

Page 18: Chapter 27 Interference and the Wave Nature of Light.

Solution• a-

Since the first bright fringe occurs when m = 0, the number of bright fringes is m+1=149

Page 19: Chapter 27 Interference and the Wave Nature of Light.

Part b

• b) Where the plates touch, there is a dark fringe because of destructive interference between the light waves represented by rays 1 and 2. Destructive interference occurs because the thickness of the wedge is zero here and the only difference between the rays is the half-wavelength phase change due to reflection from the lower plate.

Page 20: Chapter 27 Interference and the Wave Nature of Light.

Circular interference fringes

• The air wedge between a convex spherical glass surface and an optically flat plate leads to a pattern of circular interference fringes that is known as Newton’s rings.

Page 21: Chapter 27 Interference and the Wave Nature of Light.

The Michelson Interferometer

• An interferometer is an apparatus that can be used to measure the wavelength of light by utilizing interference between two light waves

Page 22: Chapter 27 Interference and the Wave Nature of Light.

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 23: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

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

Page 24: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

Page 25: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

This top view shows five sources of Huygens’ wavelets.

Page 26: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

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

Page 27: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

Dark fringes forsingle slitdiffraction

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m

Page 28: Chapter 27 Interference and the Wave Nature of Light.

27.5 Diffraction

Page 29: Chapter 27 Interference and the Wave Nature of Light.

27.6 Resolving Power

First minimum of a circular diffraction pattern

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22.1sin

diameter of hole

Page 30: Chapter 27 Interference and the Wave Nature of Light.

27.6 Resolving Power

Page 31: Chapter 27 Interference and the Wave Nature of Light.

27.6 Resolving Power

Rayleigh criterion

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

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22.1min

Page 32: Chapter 27 Interference and the Wave Nature of Light.

The Diffraction Grating

• Diffraction patterns of bright and dark fringes occur when monochromatic light passes through a single or double slit. Fringe patterns also result when light passes through more than two slits, and an arrangement consisting of a large number of parallel, closely spaced slits called a diffraction grating

Page 33: Chapter 27 Interference and the Wave Nature of Light.

27.7 The Diffraction Grating

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

Page 34: Chapter 27 Interference and the Wave Nature of Light.

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 35: Chapter 27 Interference and the Wave Nature of Light.

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 36: Chapter 27 Interference and the Wave Nature of Light.

27.7 The Diffraction Grating

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Page 37: Chapter 27 Interference and the Wave Nature of Light.

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

Page 38: Chapter 27 Interference and the Wave Nature of Light.

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

Page 39: Chapter 27 Interference and the Wave Nature of Light.

27.9 X-Ray Diffraction

Page 40: Chapter 27 Interference and the Wave Nature of Light.

27.9 X-Ray Diffraction