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Chapter 32
                                   Electromagnetic Waves


PowerPoint® Lectures for
University Physics, Twelfth Edition
 – Hugh D. Young and Roger A. Freedman

Lectures by James Pazun
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Goals for Chapter 32
 • To do an overview of Maxwell’s equations and
   electromagnetic waves
 • To study sinusoidal electromagnetic waves
 • To consider the passage of electromagnetic waves
   through matter
 • To determine the energy and momentum of
   electromagnetic waves
 • To observe wave addition, the formation of a
   standing electromagnetic wave


Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Introduction
 • If an electric field vector propagates, it
   generates a magnetic field vector. Or,
   is it the other way?
 • The “chicken and the egg” argument
   of which disturbance causes the other
   aside, this is often a favorite portion of
   a first course in physics.
   Electromagnetic waves, at least in the
   form of light, are common to many of
   our daily experiences. Even without
   vision, you can stand in the sun
   wearing a dark shirt and perceive
   electromagnetic waves.


Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Maxwell’s equations
 • After Ampere and Faraday came James Clark Maxwell. He penned
   a set of four equations that draw Gauss, Ampere, and Faraday’s
   laws together in a comprehensive description of the behavior of
   electromagnetic waves.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Electromagnetic waves are ubiquitous
 • If you tried to cite all
   the places you notice
   electromagnetic waves
   in your classroom, you
   would conclude in a
   few minutes that they
   are everywhere.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Electromagnetic waves occur over a wide range
 • Where wavelength is large, frequency is small.
 • The range extends from low energy and frequency (radio and
   television) to high energy and small wavelength (gamma rays).




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
The propagation of electromagnetic waves
 • The wave front moves at speed c, equal to 3.0 × 108 m/s.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Propagation of electromagnetic waves II




                                                                                index of
                                                                                refraction




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
The wave equation




                                                                                Electromagnetic wave
                                                                                traveling in the +x direction




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
The wave




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
The wave



                                                                                T = 1.6 s



                          horizontal axis - time axis



                                                             λ



                      horizontal axis - position axis
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
• A coating of oil on water or a
   delicate glass prism can create a
   rainbow. A rainstorm among open
   patches of daylight can cast a
   conventional rainbow. Both effects
   are beautiful and arise from the
   wavelength dependence of refraction
   angles.
 • Eyeglasses or contact lenses both use
   refraction to correct imperfections in
   the eyeball’s focus on the retina and
   allow vision correction.



Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Reflection and refraction
 • The figure below illustrates both reflection and refraction at once. The
   storefront window both shows the passersby their reflections and allows them
   to see inside.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
We will consider specular reflections
 • A real surface will scatter and reflect light. Diffuse reflection is the
   rule, not the exception. We will use specular reflection as we used
   the ray approximation, to make a very difficult problem
   manageable.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Laws of reflection and refraction
 • Angle of incidence = angle of reflection.


 • Snell’s Law of Refraction considers the
   slowing of light in a medium other than
   vacuum … the index of refraction.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Why should the ruler appear to be bent?
 • The difference in index of refraction for air and water causes your eye to
   be deceived. Your brain follows rays back to the origin they would have
   had if not bent.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Tabulated indexes of refraction




                         As index of refraction increases, velocity of
                         light in the medium decreases




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Quiz ¼ sheet of paper
1. Write down the relationship of frequency and the wavelength of light in a vacuum.
2. If an EM wave or light enters a dielectric, its frequency remains the same. As it enters
     the material, the electrons in the material vibrate with a driving frequency equal to that
     of the EM wave but its wavelength would differ.
• The speed of light in vacuum is c = 3.0 x 108 m/s, what would be its speed in water if its
  index of refraction is 1.33?
3. Write down the law of reflection and refraction (Snell’s law)
4. Knowing Snell’s law and the theory of index of refaction, rank the speed of light through
    each medium from least to greatest.




                                                                                        50o
                                                         5o                 15o   15o
                       15o                     5o                                             D
                                                                           C
                                A                   B

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Quiz (by pair) >:)




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Chapter 35
                                                                                Interference


PowerPoint® Lectures for
University Physics, Twelfth Edition
 – Hugh D. Young and Roger A. Freedman

Lectures by James Pazun
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Goals for Chapter 35
  • To consider interference and coherent
    sources
  • To study two-source interference of light
  • To determine intensity in interference
    patterns
  • To consider interference in thin films
  • To study the Michelson interferometer



Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Introduction
• Rainbows in the sky: been
  there, seen that. A thin-film
  soap bubble: why should that
  create a rainbow effect?
• This thin film is dispersing
  white light and revealing a
  r.o.y.g.b.i.v. spectrum of color.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Wave fronts from a disturbance
  • Think back to our first slide on
    wave motion when the father
    threw an object into the pool and
    the boy watched the ripples
    proceed outward from the
    disturbance. We can begin our
    discussion of interference from
    just such a scenario, a coherent
    source and the waves from it that
    can add (constructively or
    destructively).




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
A “snapshot”
• The “snapshot” of sinusoidal waves spreading out from two
  coherent sources.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
A “snapshot”
• The “snapshot” of sinusoidal waves spreading out from two
  coherent sources.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Double slit interference of light
 We consider
    Monochromatic
     Single wavelength
     Best example is laser

     Coherent
      Same frequency
      Definite constant phase relationship (not necessarily in
      phase)




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Double slit interference of light
  • Two waves interfering constructively and destructively.
  • Young did a similar experiment with light.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Double slit interference of light
  • Two waves interfering constructively and destructively.
  • Young did a similar experiment with light.




                                  L
                                                       L




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
As the waves interfere, they produce fringes




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
As the waves interfere, they produce fringes




                                                                    Constructive Interference

                                                                    Destructive Interference

                                                                    m is called the order number

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
As the waves interfere, they produce fringes




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Interference from two slits or two radio stations
 • In a two-slit interference experiment, the slits are 0.200 mm apart
   and the screen is at a distance of 1.00 m. The third bright fringe
   (not counting the central bright fringe straight ahead from the slits)
   is found to be displaced 9.49 mm from the central fringe. Find the
   wavelength of light used.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Interference between mechanical and EM waves




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Thin Film Interference




                                                                           Constructive Interference


                                                                           Destructive Interference




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Thin films will interfere




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Quiz. Understanding interference




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Chapter 36
                                                                                Diffraction


PowerPoint® Lectures for
University Physics, Twelfth Edition
 – Hugh D. Young and Roger A. Freedman

Lectures by James Pazun
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Goals for Chapter 36
 • Fresnel and Fraunhofer diffraction
 • Single-slit diffraction
 • Diffraction gratings




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Introduction
 • It’s intuitive that sound can diffract
   (and travel around corners). Light
   doesn’t “show its poker hand” so
   easily.
 • If you shine light from a point
   source to a ruler and look at the
   shadow, you’ll see the edges are …
   well … not sharp. A close
   inspection of the indistinct edge
   will reveal fringes.
 • This phenomenon may not sound
   useful yet but stay with us until the
   end of Chapter 36. This line of
   thinking has shown the way for
   advances in DVD technology and
   applications in holography.

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fresnel and Fraunhofer diffraction
 • According to geometric optics, a light source shining on an object
   in front of a screen will cast a sharp shadow. Surprisingly, this
   does not occur.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Diffraction
 • If the source and the screen are close to the edge causing the diffraction, the
   effect is called “near-field” or Fresnel diffraction. If these objects are far
   apart, so as to allow parallel-ray modeling, the diffraction is called “far-
   field diffraction” or Fraunhofer diffraction.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Diffraction from a single slit




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Dark fringes in single-slit diffraction
 • The figure illustrates Fresnel and Fraunhofer outcomes.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fresnel or Fraunhofer?
 • Differentiating Fresnel and Fraunhofer




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fraunhofer diffraction




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fraunhofer diffraction
                                                            divide source into two equal parts
                                                                         destructive interference



                                                            divide source into four equal parts




                                                                                             divide source into six equ
                                                                                and so on...
                                                                                                            eight


                                                                                   condition for destructive
                                                                                   interference
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fraunhofer diffraction




                                                                                condition for destructive
                                                                                interference


Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Fraunhofer diffraction and an example of analysis
 • A photograph of a Fraunhofer pattern from a single slit.




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Resolution




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Resolution




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Resolution




                                                                                Smaller wavelength means less
                                                                                angle to resolve object

           Why electron microscopes can see better than optical microscopes.
           Wavelength of electron is small ~10-10 m
           Light is ~10-7 m
Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
Quiz!
  1. Write down the equation for constructive
     interference for thin films given na < nb
     < nc given a light of wavelength λ
     enters the film. let m be the order
     number
              na
              nb                                            t
              nc




Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley

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Electromagnetic waves and optics

  • 1. Chapter 32 Electromagnetic Waves PowerPoint® Lectures for University Physics, Twelfth Edition – Hugh D. Young and Roger A. Freedman Lectures by James Pazun Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 2. Goals for Chapter 32 • To do an overview of Maxwell’s equations and electromagnetic waves • To study sinusoidal electromagnetic waves • To consider the passage of electromagnetic waves through matter • To determine the energy and momentum of electromagnetic waves • To observe wave addition, the formation of a standing electromagnetic wave Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 3. Introduction • If an electric field vector propagates, it generates a magnetic field vector. Or, is it the other way? • The “chicken and the egg” argument of which disturbance causes the other aside, this is often a favorite portion of a first course in physics. Electromagnetic waves, at least in the form of light, are common to many of our daily experiences. Even without vision, you can stand in the sun wearing a dark shirt and perceive electromagnetic waves. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 4. Maxwell’s equations • After Ampere and Faraday came James Clark Maxwell. He penned a set of four equations that draw Gauss, Ampere, and Faraday’s laws together in a comprehensive description of the behavior of electromagnetic waves. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 5. Electromagnetic waves are ubiquitous • If you tried to cite all the places you notice electromagnetic waves in your classroom, you would conclude in a few minutes that they are everywhere. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 6. Electromagnetic waves occur over a wide range • Where wavelength is large, frequency is small. • The range extends from low energy and frequency (radio and television) to high energy and small wavelength (gamma rays). Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 7. The propagation of electromagnetic waves • The wave front moves at speed c, equal to 3.0 × 108 m/s. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 8. Propagation of electromagnetic waves II index of refraction Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 9. The wave equation Electromagnetic wave traveling in the +x direction Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 10. The wave Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 11. The wave T = 1.6 s horizontal axis - time axis λ horizontal axis - position axis Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 12. • A coating of oil on water or a delicate glass prism can create a rainbow. A rainstorm among open patches of daylight can cast a conventional rainbow. Both effects are beautiful and arise from the wavelength dependence of refraction angles. • Eyeglasses or contact lenses both use refraction to correct imperfections in the eyeball’s focus on the retina and allow vision correction. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 13. Reflection and refraction • The figure below illustrates both reflection and refraction at once. The storefront window both shows the passersby their reflections and allows them to see inside. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 14. We will consider specular reflections • A real surface will scatter and reflect light. Diffuse reflection is the rule, not the exception. We will use specular reflection as we used the ray approximation, to make a very difficult problem manageable. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 15. Laws of reflection and refraction • Angle of incidence = angle of reflection. • Snell’s Law of Refraction considers the slowing of light in a medium other than vacuum … the index of refraction. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 16. Why should the ruler appear to be bent? • The difference in index of refraction for air and water causes your eye to be deceived. Your brain follows rays back to the origin they would have had if not bent. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 17. Tabulated indexes of refraction As index of refraction increases, velocity of light in the medium decreases Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 18. Quiz ¼ sheet of paper 1. Write down the relationship of frequency and the wavelength of light in a vacuum. 2. If an EM wave or light enters a dielectric, its frequency remains the same. As it enters the material, the electrons in the material vibrate with a driving frequency equal to that of the EM wave but its wavelength would differ. • The speed of light in vacuum is c = 3.0 x 108 m/s, what would be its speed in water if its index of refraction is 1.33? 3. Write down the law of reflection and refraction (Snell’s law) 4. Knowing Snell’s law and the theory of index of refaction, rank the speed of light through each medium from least to greatest. 50o 5o 15o 15o 15o 5o D C A B Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 19. Quiz (by pair) >:) Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 20. Chapter 35 Interference PowerPoint® Lectures for University Physics, Twelfth Edition – Hugh D. Young and Roger A. Freedman Lectures by James Pazun Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 21. Goals for Chapter 35 • To consider interference and coherent sources • To study two-source interference of light • To determine intensity in interference patterns • To consider interference in thin films • To study the Michelson interferometer Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 22. Introduction • Rainbows in the sky: been there, seen that. A thin-film soap bubble: why should that create a rainbow effect? • This thin film is dispersing white light and revealing a r.o.y.g.b.i.v. spectrum of color. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 23. Wave fronts from a disturbance • Think back to our first slide on wave motion when the father threw an object into the pool and the boy watched the ripples proceed outward from the disturbance. We can begin our discussion of interference from just such a scenario, a coherent source and the waves from it that can add (constructively or destructively). Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 24. A “snapshot” • The “snapshot” of sinusoidal waves spreading out from two coherent sources. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 25. A “snapshot” • The “snapshot” of sinusoidal waves spreading out from two coherent sources. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 26. Double slit interference of light We consider Monochromatic Single wavelength Best example is laser Coherent Same frequency Definite constant phase relationship (not necessarily in phase) Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 27. Double slit interference of light • Two waves interfering constructively and destructively. • Young did a similar experiment with light. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 28. Double slit interference of light • Two waves interfering constructively and destructively. • Young did a similar experiment with light. L L Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 29. As the waves interfere, they produce fringes Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 30. As the waves interfere, they produce fringes Constructive Interference Destructive Interference m is called the order number Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 31. As the waves interfere, they produce fringes Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 32. Interference from two slits or two radio stations • In a two-slit interference experiment, the slits are 0.200 mm apart and the screen is at a distance of 1.00 m. The third bright fringe (not counting the central bright fringe straight ahead from the slits) is found to be displaced 9.49 mm from the central fringe. Find the wavelength of light used. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 33. Interference between mechanical and EM waves Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 34. Thin Film Interference Constructive Interference Destructive Interference Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 35. Thin films will interfere Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 36. Quiz. Understanding interference Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 37. Chapter 36 Diffraction PowerPoint® Lectures for University Physics, Twelfth Edition – Hugh D. Young and Roger A. Freedman Lectures by James Pazun Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 38. Goals for Chapter 36 • Fresnel and Fraunhofer diffraction • Single-slit diffraction • Diffraction gratings Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 39. Introduction • It’s intuitive that sound can diffract (and travel around corners). Light doesn’t “show its poker hand” so easily. • If you shine light from a point source to a ruler and look at the shadow, you’ll see the edges are … well … not sharp. A close inspection of the indistinct edge will reveal fringes. • This phenomenon may not sound useful yet but stay with us until the end of Chapter 36. This line of thinking has shown the way for advances in DVD technology and applications in holography. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 40. Fresnel and Fraunhofer diffraction • According to geometric optics, a light source shining on an object in front of a screen will cast a sharp shadow. Surprisingly, this does not occur. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 41. Diffraction • If the source and the screen are close to the edge causing the diffraction, the effect is called “near-field” or Fresnel diffraction. If these objects are far apart, so as to allow parallel-ray modeling, the diffraction is called “far- field diffraction” or Fraunhofer diffraction. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 42. Diffraction from a single slit Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 43. Dark fringes in single-slit diffraction • The figure illustrates Fresnel and Fraunhofer outcomes. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 44. Fresnel or Fraunhofer? • Differentiating Fresnel and Fraunhofer Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 45. Fraunhofer diffraction Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 46. Fraunhofer diffraction divide source into two equal parts destructive interference divide source into four equal parts divide source into six equ and so on... eight condition for destructive interference Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 47. Fraunhofer diffraction condition for destructive interference Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 48. Fraunhofer diffraction and an example of analysis • A photograph of a Fraunhofer pattern from a single slit. Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 49. Resolution Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 50. Resolution Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 51. Resolution Smaller wavelength means less angle to resolve object Why electron microscopes can see better than optical microscopes. Wavelength of electron is small ~10-10 m Light is ~10-7 m Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley
  • 52. Quiz! 1. Write down the equation for constructive interference for thin films given na < nb < nc given a light of wavelength λ enters the film. let m be the order number na nb t nc Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley