Single Slit Diffraction

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Wave Nature of Light  Refraction  Interference  Young’s double slit experiment  Diffraction  Single slit diffraction  Diffraction grating.
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Presentation transcript:

Single Slit Diffraction

Reminder: What is Diffraction? Bending and spreading of a wave into a region behind an obstruction Examples: waves passing through openings or around corners Effects depend on how wide the opening is relative to wave length Wide opening: little wave spreading Narrow opening: wave fans out, changes shape (Wide: opening > wave length; Narrow: opening ~ wavelength

Diffraction: Why does it occur? According to Huygens’ principle, each point on a wavefront serves as a source of the next wavefront After passing through an aperture, there will be locations where the wavelets interfere constructively and destructively http://id.mind.net/~zona/mstm/physics/waves/propagation/huygens3.html With light, this will result in bright and dark fringes Destructive interference occurs when the difference in path length from two sources is half a wavelength

Interference Reminders Constructive interference (bright fringes): difference in path length = nλ phase difference = 2nπ radians Destructive interference (dark fringes): difference in path length = (n + ½)λ phase difference = (n + ½)π radians

How single slit pattern is achieved Use monochromatic, uncollimated, incoherent light: Lens 1 produces parallel wave fronts passing through slit (collimated) Lens 2 focuses pattern on screen Use a laser as the source: produces collimated coherent light 2nd lens focuses fringe patterns on screen Source of monochromatic light located at focal point of lens Laser produces coherent light: constant phase difference between sources of between individual waves

Definitions Monochromatic light: light waves all have same wavelength (or frequency) Collimated light: all waves are parallel to each other http://en.wikipedia.org/wiki/Collimated_light Coherent light: constant phase difference between sources of individual waves Laser light is coherent All wavelets on a given wavefront are, by definition, coherent http://schools.matter.org.uk/content/Interference/coherent.html

Intensity of central fringe is much greater than the rest Width of central maximum is twice that of the others

Circular Aperture Diffraction Pattern Central maximum is much brighter and wider than the rest This pattern is called an Airy disk http://www.youtube.com/watch?v=Wy3oR6fY6W8 That’s all, folks!

Derivation of Single Slit Diffraction Equation: the Setup REQUIRED DERIVATION! First dark fringe: occurs for destructive interference L

Consider wavelets arising from the top of the slit and from the center of the slit If the difference in path length between the two is λ/2, there will be destructive interference, resulting in a dark fringe From the geometry sin θ = λ/2 b/2 We also consider all of the other symmetrically placed wavelets along entire slit b/2 ~90º λ/2 Remember that all wavelets arising from the same wavefront are coherent.

Derivation (cont.) Assuming θ is small: sin θ ≈ θ Final result: θ = λ/b This the angular distance from the central maximum to first dark fringe It is also half of central maximum angle: To find the total angular displacement of the central maximum, multiply by 2 Remember: this angle has units of radians! Angle theta will be small if the wavelength is small compared to the slit width.

tan θ = d/L θ ≈ d/L Then λb ≈ d/L Distance on screen from middle of central maximum to first dark fringe: tan θ = d/L d = half-width of the central maximum projected on the screen L = distance from slit to screen If θ is small (as it will be if L >> d), then θ ≈ d/L Then λb ≈ d/L b d d would also be the distance between subsequent fringes. Angle theta will be small if the distance to the screen is large.

Single Slit Diffraction Applets What happens to fringe width when you change wavelength, slit width, and distance to screen? http://www.walter-fendt.de/ph14e/singleslit.htm http://surendranath.tripod.com/Applets/Optics/Slits/SingleSlit/SS.html http://lectureonline.cl.msu.edu/~mmp/kap27/Gary-Diffraction/app.htm A narrower slit has a wider central maximum. This can be tied back to the uncertainty principle! See http://www.youtube.com/watch?v=KT7xJ0tjB4A

Example Problem #1 Light from a laser is used to form a single slit diffraction pattern. The width of the slit is 0.10 mm and the screen is placed 3.0 m from the slit. The width of the central maximum is measured as 2.6 cm. (Hint: this is 2d) What is the wavelength of the laser light?

Answer Since the screen is far from the slit we can use the small angle approximation such that d/L = λ/b, so λ = db/L d, the half width of the center maximum is 1.3 cm so we have λ = (1.3 x 10-2 m) x (0.10 x 10-3 m) / 3.0 m λ = 430 x 10-9 m or 430 nm

Example Problem #2 Light of λ = 500 nm is diffracted by a single slit 0.05 mm wide. Find the angular position of the 1st minimum. If a screen is placed 2 meters from the slit, find the half-width of the central bright fringe. Answer: 0.01 rad; 2 cm

Example Problem #3 When light of λ = 440 nm is diffracted through a single slit, the angular position of the 1st minimum is at 0.02 rad. Find the slit width. Answer: 0.022 mm