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Chapter 37

Interference and Diffraction. Chapter 37. =. +. Combination of Waves. In general, when we combine two waves to form a composite wave, the composite wave is the algebraic sum of the two original waves, point by point in space [Superposition Principle].

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Chapter 37

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  1. Interference and Diffraction Chapter 37

  2. = + Combination of Waves In general, when we combine two waves to form a composite wave, the composite wave is the algebraic sum of the two original waves, point by point in space [Superposition Principle]. When we add the two waves we need to take into account their: Direction Amplitude Phase

  3. = + Constructive interference (Waves almost in phase) Combination of Waves The combining of two waves to form a composite wave is called: Interference The interference is constructive if the waves reinforce each other.

  4. (Waves almost cancel.) = + Destructive interference (Close to pout of phase) Combination of Waves The combining of two waves to form a composite wave is called: Interference The interference is destructive if the waves tend to cancel each other.

  5. = + Constructive interference (In phase) = + (Waves cancel) Destructive interference ( pout of phase) Interference of Waves

  6. 1 * 2 Mirror = + Interference of Waves When light waves travel different paths, and are then recombined, they interfere. Each wave has an electric field whose amplitude goes like: E(s,t) = E0 sin(ks-t) î Here s measures the distance traveled along each wave’s path. Constructive interference results when light paths differ by an integer multiple of the wavelength: s = m 

  7. 1 * 2 Mirror = + Interference of Waves When light waves travel different paths, and are then recombined, they interfere. Each wave has an electric field whose amplitude goes like: E(s,t) = E0 sin(ks-t) î Here s measures the distance traveled along each wave’s path. Destructive interference results when light paths differ by an odd multiple of a half wavelength: s = (2m+1) /2

  8. Interference of Waves Coherence: Most light will only have interference for small optical path differences (a few wavelengths), because the phase is not well defined over a long distance. That’s because most light comes in many short bursts strung together. Incoherent light: (light bulb) random phase “jumps”

  9. Incoherent light: (light bulb) random phase “jumps” Laser light is an exception: Coherent Light: (laser) Interference of Waves Coherence: Most light will only have interference for small optical path differences (a few wavelengths), because the phase is not well defined over a long distance. That’s because most light comes in many short bursts strung together.

  10. Thin Film Interference We have all seen the effect of colored reflections from thin oil films, or from soap bubbles. Film; e.g. oil on water

  11. Thin Film Interference We have all seen the effect of colored reflections from thin oil films, or from soap bubbles. Rays reflected off the lower surface travel a longer optical path than rays reflected off upper surface. Film; e.g. oil on water

  12. Thin Film Interference We have all seen the effect of colored reflections from thin oil films, or from soap bubbles. Rays reflected off the lower surface travel a longer optical path than rays reflected off upper surface. Film; e.g. oil on water If the optical paths differ by a multiple of , the reflected waves add. If the paths cause a phase difference , reflected waves cancel out.

  13. 1 2 n = 1 oil on water optical film on glass soap bubble n > 1 t Thin Film Interference Ray 1 has a phase change of  upon reflection Ray 2 travels an extra distance 2t (normal incidence approximation) Constructive interference: rays 1 and 2 are in phase  2 t = m n + ½ n  2 n t = (m + ½)  [n = /n] Destructive interference: rays 1 and 2 are  out of phase  2 t = m n  2 n t = m 

  14. 1 2 n = 1 oil on water optical film on glass soap bubble n > 1 t Thin Film Interference When ray 2 is in phase with ray 1, they add up constructively and we see a bright region. Different wavelengths will tend to add constructively at different angles, and we see bands of different colors. Thin films work with even low coherence light, as paths are short When ray 2 is  out of phase, the rays interfere destructively. This is how anti-reflection coatings work.

  15. Mirrors Input Output Beam-splitter Michelson Interferometer A Michelson interferometer uses a beam splitter to create two different optical paths. This can be used for optical testing. What is the output?

  16. Mirrors Input Output Beam-splitter Michelson Interferometer A Michelson interferometer uses a beam splitter to create two different optical paths. This can be used for optical testing. What is the output? - If the output beams are perfectly aligned, they will interfere uniformly, giving either a bright or dark output, depending on their relative phase.

  17. Input Output Michelson Interferometer But usually the beams will be a little misaligned: Interference of misaligned beams:

  18. Input Output Michelson Interferometer But usually, the beams will be a little misaligned: Interference of misaligned beams: (the lines represent maxima)

  19. Input Output Michelson Interferometer But usually, the beams will be a little misaligned: Interference of misaligned beams: (the lines represent maxima)

  20. Input Output Michelson Interferometer But usually, the beams will be a little misaligned: Interference of misaligned beams: (the lines represent maxima) Regions of high intensity

  21. Input Output S Regions of high intensity Michelson Interferometer But usually, the beams will be a little misaligned: Interference of misaligned beams: (lines = maxima) “Fringes”

  22. Optical window to be tested Mirrors Input Output Optical Testing With aMichelson Interferometer A Michelson interferometer uses a beam splitter to create two different optical paths. This can be used for optical testing.

  23. Optical window to be tested Mirrors Input Output Optical Testing With aMichelson Interferometer A Michelson interferometer uses a beam splitter to create two different optical paths. This can be used for optical testing. If the window distorts the waves, this will show up in the interference fringes: Good window.

  24. Optical window to be tested Mirrors Input Output Optical Testing With aMichelson Interferometer A Michelson interferometer uses a beam splitter to create two different optical paths. This can be used for optical testing. If the window distorts the waves, this will show up in the interference “fringes”: Good window. Bad window

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