1. April 18 Physics 54 Lecture Professor Henry Greenside

2. Key Points from Previous Lecture Sign conventions for d o, d i, f, m, h i

3. Today’s Topics Chapter 35: “The Wave Nature of Light: Interference” Huygens's principle Young’s double-slit experiment which demonstrates that light is a wave and that the wave is transverse. Interference in thin films. How f and for light change in a new medium. Applications of thin films: non-reflective coatings, measuring thickness of small wires.

4. Chapter 35: Interference of Waves Please review Sections 15-6 through 15-8 of Volume I Giancoli.

5. Huygens’ Principle Explains Diffraction Waves in isotropic medium r = v t

6. Huygens' Principle Huygens’ Principle can be used to: 1.Explain the law of reflection. 2.Explain refraction of waves at an interface. 3.Explain diffraction of waves around a corner. As you might expect, the heuristic idea of Huygens can be fully justified through various derivations associated with the Maxwell equations.

7. Applying Huygens’ Principle to Two Slits

8. To Understand Interference, Understand Superposition of Waves Nota bene: it is the relative phase that counts here.

9. Interference of Coherent Waves In the Double-Slit Experiment Waves at slits have to be coherent for interference to occur! Two different light bulbs in front of each slit will not give interference pattern.

10. Light Particles or Waves? Young’s Double-Slit Experiment! particleswaves

11. Interference Preconditions 1.Light must be monochromatic, i.e., involve just a single frequency and single wavelength. 2.Light sources must be coherent, the relative phase is always the same. 3.Light sources must have the same amplitudes. If these conditions do not hold, one still gets constructive and destructive interference but the interference pattern can change with time or not be complete (destructive interference leads to a decrease in amplitude but not to zero amplitude).

12. Conditions for Constructive and Destructive Interference of Two Coherent Waves Constructive and destructive interference (of two coherent monochromatic equal-amplitude waves emitted from sources S1 and S2) occur at point P in space when difference  l in distances l 1 and l 2 of P to sources S1 and S2 respectively satisfies:  l = l 1 – l 2 = m constructive  l = l 1 – l 2 = (m-1/2) destructive where is wavelength of waves and m is any integer. For points for which these conditions don’t hold, you get intermediate results, partial constructive or partial destructive interference.

13. Two-slit Experiment: Light, Electrons Are Neither Waves Nor Particles Akira Tonomura http://www.pnas.org/content/vol0/issue2005/images/data/0504720102/DC1/04720Movie1.mpg

14. m is the order of an interference fringe Whiteboard: Derivation of Criteria for Dark and Light Bands in Young Expt

15. Proving that Light is a Transverse Wave: Two- slit Experiment Plus Two Linear Polarizers Consider Young’s double-slit interference experiment but now put a linear polarizing filter in front of each slit. Then as transmission axis of one polarizer is slowly rotated about its axis while transmission axis of other polarizer is kept fixed, one finds experimentally that the bright regions become dimmer, the dark regions become brighter, until the fringes disappear into a smoothly varying region that is brightest behind the slits and gets dimmer off to the sides. This proves that light is transverse, i.e., can be polarized. What is happening is that the light that is polarized vertically can not interfere with light that is polarized horizontally since the E vectors can’t line up to cancel to zero.

16. PRS Question: If distance d between slits is decreased, then the angles  corresponding to the bright fringes will 1.all become smaller. 2.all become larger 3.some will become larger, some smaller. 4.remain unchanged but the fringes will all become dimmer. 5.remain unchanged but the fringes will all become brighter.

17. Worked Example at Whiteboard A screen contains two slits distance d = 0.100 mm apart and is length L = 1.20 m from a viewing screen. Monochromatic light of wavelength = 500 nm falls on the slits from a distant source. About how far apart  x will the bright interference fringes be on the screen? Answer: About 6 mm. Use small angle approximations to simplify algebra, avoid using sin and tan functions.

18. PRS Question: If wavelength of monochromatic light impinging on two- slits experiment increases, then bright fringes 1.all become closer. 2.all spread further apart. 3.some become closer, some further apart.

19. Wavelengths of Light From Double-Slit Interference White light (not monochromatic light) impinges on slits two slits are distance d = 0.50 mm apart screen is length L = 2.5 m away. Violet and red m=1 fringes are 2.0 and 3.5 mm from central fringe. What are the wavelengths of the violet and red light? Answers: 400 nm and 700 nm respectively.

20. Application of Interference: Thin Films

21. Thin Film Interference Versus Two-Slit Interference Two-slit interference involves light from two separate sources S 1 and S 2. Thin-film interference involves light from single source that interferes with itself by reflecting off different interfaces between two different media, which then produces different sources of light that interfere with each other. Thin-film interference of great importance in optics, precision machinery, and biology.

22. Whiteboard Discussion of Thin-Film Interference 1.Review how wave on rope reflects at interface between less dense and more dense sections of rope. Can get inversion of wave which corresponds to a shift of wave by ½ wavelength. 2.Same occurs for light: when light passes from less dense medium (vacuum or air) to more dense medium, reflected light will be shifted by ½ wavelength. 3.Need to understand index of refraction n that characterizes how light behaves in a medium. Speed slows down to c/n < c, wavelength decreases to n = /n, and frequency is unchanged as light passes into new medium. 4.Criterion for bright reflection (constructive interference) is then the usual one: difference in distances traveled must be integer multiple of wavelength n in the medium. Get no reflection (destructive interference) if difference in distances traveled is half-integer multiple of wavelength n.

23. Section 15-7 on Waves: Reflection When wave hits discontinuity, part is reflected and part is transmitted. If new medium is “stiffer”, wave inverts ( /2 shift in wavelength,  /2 shift in phase)

24. Light Reflection From Denser Media: /2 Shift In Position of Wave Inversion with /2 shift in position No inversion

25. Measure Small Thicknesses with Air Wedge

26. Interference From Thin Film Count total number of half-wavelength shifts: 1.One at air-oil interface. 2.One at oil-water interface. Two inversions cancel each other so get constructive interference when difference in length of paths is integer multiple of wavelength n in the oil! Next get total extra length of path 2t that light traverses.

27. What is minimum thickness t of soap bubble if it appears green ( =540 nm) at the point of front surface closest to viewer? Assume n soap = 1.35. Solution: Total number of inversions (phase shifts of /2) is 1 so criterion for constructive interference: Get smallest t for m = 0, gives answer t=100 nm. Worked Example 35-7: Thickness of Soap Bubble Skin

28. PRS: How Many Phase Shifts In Example 35-8? n air = 1, n MgF2 = 1.38 n glass = 1.50